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ACKNOWLEDGEMENTS



IN THE NAME OF ALLAH, THE MOST GRACIOUS, THE MOST MERCIFUL

Firstly, I am grateful to Allah S.W.T for giving me the strength to complete this project
successfully. I would like to express my gratitude Associated Professor Maheran
Nuruddin for the guidance and support to this report.

Special thanks to my family, especially my parent who always support and pray for my
success. I wish to thank my friends for their support. They have been very supportive
throughout the completion of this project.

Last but not least, thank you again for those who spent time and effort with me in
completing this report, directly or indirectly. Without Allah bless and the all kindness of
these people, I will never succeed in completing this project. Thank you so much.
Wasalam.
TABLE OF CONTENTS

ACKNOWLEDGEMENTS ................................................................................................. i
TABLE OF CONTENTS .................................................................................................... ii
LIST OF TABLES ............................................................................................................. iii
LIST OF FIGURES ........................................................................................................... iii
ABSTRACT ....................................................................................................................... iv
1. INTRODUCTION ........................................................................................................ 1
2. METHODOLOGY ....................................................................................................... 4
3. IMPLEMENTATION ................................................................................................... 6
4. RESULTS AND DISCUSSION ................................................................................. 32
5. CONCLUSIONS AND RECOMMENDATIONS ..................................................... 33
REFERENCES ................................................................................................................. 34




                                                                ii
LIST OF TABLES
Table 1. Fourier series calculation by using excel for dengue cases in Shah Alam (2009) . 8
Table 2. Fourier series calculation by using excel for dengue cases in Gombak (2009) ... 12
Table 3. Fourier series calculations by using excel for dengue cases in Klang (2009) ..... 16
Table 4. Fourier series calculations for dengue cases in Shah Alam (2010) ..................... 20
Table 5. Fourier series calculations by using excel for dengue cases in Gombak (2010) . 24
Table 6. Fourier series calculations by using excel for dengue cases in Klang (2010) ..... 28
Table 7. Fourier series equations on 1st harmonic for 2009 .............................................. 32
Table 8. Fourier series equations on 1st harmonic for 2010 .............................................. 32
Table 9. Analysis from graph using maple software for 2009 ........................................... 32
Table 10. Analysis from graph using maple software for 2010 ......................................... 32




                                       LIST OF FIGURES

Figure 1. Graph of dengue cases in Shah Alam, Gombak and Klang for year 2009 ........... 6
Figure 2. Graph of dengue cases in Shah Alam, Gombak and Klang for year 2010 ........... 7
Figure 3. Fourier series graph plotted for dengue cases in Shah Alam (2009) .................. 11
Figure 4. Fourier series graph plotted for dengue cases in Gombak (2009) ...................... 15
Figure 5. Fourier series graph plotted for dengue cases in Klang (2009) .......................... 19
Figure 6. Fourier series graph plotted for dengue cases in Shah Alam (2010) .................. 23
Figure 7. Fourier series graph plotted for dengue cases in Gombak (2010) ...................... 27
Figure 8. Fourier series graph plotted for dengue cases in Klang (2010) .......................... 31




                                                    iii
ABSTRACT

Dengue is the most dangerous mosquito virus infection to the human in the world. Up to
100 million cases are reported annually and some two billion people are at risk of
infection in the world. There is no specific cure or medicine to shorten the course of
dengue. The occurrence of dengue in Malaysia has become more serious year to year.
The aims of this study are to know the pattern of dengue cases that happened in chosen
district and to obtain the highest point for dengue cases in chosen district by referring to
Fourier series graph plotted. This project focuses on certain districts which had
recorded the highest dengue cases among district in Malaysia which are Shah Alam,
Gombak and Klang. It is difficult to determine and predict the dengue cases for the next
year by following the trend line that is generated by Excel. Thus, the alternative that we
have is to transform the graph into a periodic graph using Fourier series, so that the
highest point for the dengue cases can be determined. Fourier series is an expansion of a
periodic function of period which the base is the set of sine functions. Hence, Fourier
series is one of the alternative methods to compare and explain the pattern of dengue
cases recorded. The result between year 2009 and 2010 show the number of dengue cases
seasonally peak at first quarter of year which averagely recorded in period week 7 to
week 14 (February to April).




                                             iv
1.     INTRODUCTION

Dengue is the most dangerous mosquito virus infection to the human in the world. Ang
and Li (1999) stated that up to 100 million cases are reported annually and some two
billion people are at risk of infection in the world. Dengue viruses are transmitted from
vector (mosquitoes) to the susceptible human beings by various mosquitoes such as
Aedes aegypti and Aedes albopictus. From that, the infected person will have a few
symptoms such as high fever (40°C), chills, headache, pain in the eyes, deep muscle and
joint pains and extreme fatigue. Actually, the infected person will have high fever for two
to four days. Then, the body temperature will drop rapidly and intense sweating takes
places. But, patient’s body will show up small red bumps. These are a few symptoms that
will happen to the infected person. If the patient does not take immediately treatment,
dengue may cause death.

Knowing how dengue being transmitted is very important. This is relevant to this study
because we must identify and know who is the vector and the host. Basically, dengue
viruses are transmitted from the vector (mosquitoes) to the host (humans). The
transmitted dengue virus process happened by mosquitoes bite during mosquitoes blood
feeding. The mosquitoes also may carry the virus from one host to another host. When
the virus has been transmitted to the host (humans) incubation period will occur. The
dengue viruses multiply during incubation time. After three to five days, the symptoms
of dengue will appear and attack patients.

There is no specific cure or medicine to shorten the course of dengue. Actually, the
medicine provided by doctors is to reduce and alleviate the symptoms and sign of dengue.
In this situation, the patient (infected person) takes paracetamol to relieve muscle and
joint aches, fever and headache. The patient is advice to keep rest in a screened room to
prevent mosquitoes from entering. The dengue virus will be transmitted to another host
(human) if the patient is bitten second times. After this treatment, in a few days, we can
define the patient is fully recovered and in the best condition (recover person) when the
symptoms had disappeared.

The occurrence of dengue in Malaysia had become more serious year to year. The
Ministry of Health Malaysia (2009) stated that dengue has become pandemic. Besides
that, people did not take this problem as a serious problem. In order to increase the
people’s sensitivity of dengue, the Ministry of Health has done many activities and
campaign such as advertisement through the television and internet. The activities and
campaign also include involvement of students in primary and secondary schools. For
example, the competition “AntiAedes Ranjer Ridsect” organized by Sara Lee Company
(Ridsect) which cooperated with Ministry of Health Malaysia.




                                            1
In order to analyze the dengue cases which happened in Malaysia for this study, Fourier
series was choose because of its availability to present and show the new perspective
analysis of dengue cases. Zill and Cullen (2009) stated that the representation of a
function in the form of a series is widely and frequently used to solve and explain the
common problem situation.

The history of Fourier series started when Bernoulli, D’ Allembert and Euler (1750) had
used and introduced the idea of expanding a function in the form a series to solve the
associated with the vibration of strings. Then, Joseph Fourier who a French physicist,
(1768-1830) improved and developed the approach of Fourier series where it was
generally useful nowadays. However, the search had done by Joseph Fourier gave impact
to all mathematicians and physicists at that time such as Laplace, Poisson and Lagrange.
They doubt and debate about Fourier’s work because it opposite and inversed to their
idea. But, the text of Joseph Forier which Theorie Analytique de la Chaleur (The
Analytical Theory of Heat) become the source for the modern method in order to solve
problems associated with partial differential equations subject to prescribed boundary
conditions.

Nowadays, the application of Fourier series analysis is commonly used in physic and
electrical engineering sector which how frequency associated to a dynamical systems.
The text from Joseph Fourier influenced in created electrical component such as
electronic rectifiers. Fourier series also is the best method to analyze the data series such
as dengue cases which useful to compare and determine the dengue cases happened in
Malaysia.

Angove (2009) analyze the periodic time domain voltage waveform and convert it to the
frequency domain which always uses in electronic communication systems. For example
a waveform usually decomposed into sum of harmonically related sine, cosine waveform
and constant which is known as Fourier series.

Klingenberg (2005) showed the way to apply and calculate Fourier series analysis by
using Microsoft Excel. Excel generally shows the magnitude versus time is known
waveform. Klingenberg (2005) done the experiments call for the “harmonic content” of a
reproduced waveform is a display of the magnitude of the waveform (Y-axis) versus the
frequency (X-axis). In other word, we called it as frequency spectrum and it allows
visualizing a waveform according to its frequency content.

Kvernadzi, Hagstrom and Shapiro (1999) studied about the utilization of the truncated
Fourier series and it applies as a tool for the approximation of the points of discontinuities
and the magnitudes by using integrals. Abas, Daud and Yusuf (2009) studied about
rainfall by using Fourier series with significant number of harmonics is fitted to the
model’s parameter. The results of their studies showed that statistical properties of the
estimated rainfall series were able to match most of those of the historical series. The
Fourier series makes the model more parsimony by grabs the seasonal fluctuations within
the model.




                                              2
The strategy or plan must be systematic. So, modeling how dengue spread among
population localized in a district guides the Ministry of Health Malaysia to prevent these
epidemics become more danger to community. The model were showed the seasonal
pattern that are useful in prevent in a spread of dengue. Favier (2006) suggest that,
statistical analyses of longitudinal surveys sites are needed before choose the right
parameters.

The scope of this study was in small scale because Favier, Degallier and Dubois (2005)
stated that possibility of transmission dengue also depends on the population density and
previous immunization. Sometimes, factor likes rainfalls, temperature must be
considered. The virus progression occurs at a daily scale; therefore it must be recorded in
weeks or days to be more accurate and precise. So, the prediction and modeling of
dengue repartition and dynamics raises must different depends on the situation and place.
Since the scope of study is in small scale, the result will be more accurate. For instance,
modeling of dengue prevalence is conceivable at town-scale like Shah Alam, Subang and
Klang but not at global scale, where long-range interactions cannot model accurately.

Dengue will impact high death rate if we are not able to control it. Being able to know
the pattern and trend of dengue cases will be of great significant in reducing the death rate
that will cause by dengue. A good and reliable mathematical modeling about pattern and
trend dengue will help the government to take preventing control and precaution control
to reduce the dengue case in certain time in the future since this disease does not have
specific treatment.

The objectives of this study are to know the pattern of dengue cases that happened in
chosen district, to obtain the first harmonic equation of Fourier series and compare the
peak value for dengue cases in the chosen district by referring to Fourier series graph
plotted. This project focuses on certain districts which had recorded the highest dengue
cases among district in Malaysia which are Shah Alam, Gombak and Klang.




                                             3
2.       METHODOLOGY

Some of Fourier series formula from Zill and Cullen (2009) that are used throughout this
study is given as follows:-

The Fourier series of a function f defined on the interval [0, 2L] is given by:
               a      
                               n             n 
       f ( x)  0    a n cos     x  bn sin    x
                2 n1           L              L 

where,
                    2L
                1
         a0 
                L    f ( x)dx
                       0

                                      n
                    2L
                1
         an 
                L       f ( x) cos
                       0
                                       L
                                         xdx

                                      n
                    2L
                1
         bn 
                L    f ( x) sin
                    0
                                       L
                                         xdx



Fourier series determined from the coefficient which are a0, an, and bn. Since, we are
focus on the first harmonic term, we can write these coefficients as follow:
                2L
              1
        a 0   f ( x)dx
              L 0
                1 
                  yk
                L k 1
                

                y         k
               k 1

               L
            [average of f ( x)]


                                      n
                    2L
                1
         a1 
                L    f ( x) cos
                    0
                                       L
                                         xdx

                1             nx  
                   y k  cos
                                      
                                        
                L  k 1        L  
                         nx  
               y k  cos
                                 
                                   
              k 1        L  
           
                        L




                                               4
n
                   2L
               1
       b1 
               L    f ( x) sin
                   0
                                   L
                                     xdx

               1              nx  
                  y k  sin 
                                      
                                        
               L  k 1         L  
                          nx  
               y k  sin 
                                  
                                    
              k 1         L  
           
                        L

where yk is data obtained from the dengue cases and 2L is the period time. Then, we
arrange the Fourier series as follow:
                a           x       x          2x          2x 
        f ( x)  0   a1 cos  b1 sin    a2 cos      b2 sin       ...
                 2           L       L            L            L 

                     x          x 
The term of  a1 cos  b1 sin  is called the first harmonic. We can write the sum of
                      L           L
sine and cosine term, with the same periodic as follow:
                                 x             2x       
        y  f ( x)  c0  c1 sin  1   c2 sin       2   ...
                                L               L         
where,
             a
        c0  0 ,
              2
       c1  a12  b12 ,
                         a1 
        1  tan 1 
                            
                             
                         b1 

In this study, we focus on the first harmonic term on this equation which is:
                         x      
         y  c0  c1 sin
                         L   1 
                                  
                                 

This equation is plotted by using Maple software to determine the peak value and analyze
the trend of dengue cases.




                                             5
3.     IMPLEMENTATION

Before proceed to Fourier series method, the data of dengue case were plotted by using
Excel in order to look for the pattern of dengue cases which happened in Shah Alam,
Gombak and Klang.

     Figure 1. Graph of dengue cases in Shah Alam, Gombak and Klang for year 2009




Figure1 shows that comparison of dengue cases between Shah Alam, Gombak and Klang
since 7 January until 26 December 2009 by graph. From the graph above, it is hard to
compare the pattern between these districts. Thus, it is not accurate if we want to
generate the prediction for the next year based on the trend line equation. Furthermore,
there are a lot of scatter plot dengue cases data that fluctuations over the period cover.




                                            6
Figure 2. Graph of dengue cases in Shah Alam, Gombak and Klang for year 2010




Figure2 shows that comparison of dengue cases between Shah Alam, Gombak and Klang
since 9 January until 8 August 2010 by graph. From the graph above, it is hard to
compare the pattern between these districts. Thus, it is not accurate if we want to
generate the prediction for the next year based on the trend line equation. Furthermore,
there are a lot of scatter plot dengue cases data that fluctuations over the period cover.

So, more suitable method to compare the pattern of number of dengue cases recorded in
Shah Alam, Gombak and Klang is Fourier series.




                                            7
Table 1. Fourier series calculation by using excel for dengue cases in Shah Alam (2009)
   Week (x)   Cases (y)   (πx)/L   cos (πx/L)   sin (πx/L)   [cos ((πx)/L)] *yk   [sin ((πx)/L)] *yk
      1         244       0.1232     0.9924       0.1229          242.1506              29.9847
      2         425       0.2464     0.9698       0.2439          412.1637            103.6633
      3         362       0.3696     0.9325       0.3612          337.5549            130.7695
      4         360       0.4928     0.8810       0.4731          317.1644            170.3137
      5         474       0.6160     0.8162       0.5778          386.8773            273.8648
      6         337       0.7392     0.7390       0.6737          249.0460            227.0354
      7         525       0.8624     0.6506       0.7594          341.5746            398.6876
      8         482       0.9856     0.5524       0.8336          266.2399            401.7963
      9         489       1.1088     0.4457       0.8952          217.9661            437.7348
     10         608       1.2320     0.3324       0.9432          202.0717            573.4379
     11         521       1.3552     0.2139       0.9768          111.4591            508.9380
     12         622       1.4784     0.0923       0.9957           57.3909            619.3467
     13         552       1.6016    -0.0308       0.9995          -16.9989            551.7382
     14         383       1.7248    -0.1534       0.9882          -58.7490            378.4674
     15         260       1.8480    -0.2737       0.9618          -71.1524            250.0747
     16         360       1.9712    -0.3898       0.9209         -140.3229            331.5260
     17          41       2.0944    -0.5000       0.8660          -20.5000              35.5070
     18         132       2.2176    -0.6026       0.7980          -79.5478            105.3383
     19         127       2.3408    -0.6961       0.7179          -88.4090              91.1748
     20          76       2.4640    -0.7791       0.6269          -59.2101              47.6462
     21         102       2.5872    -0.8502       0.5264          -86.7221              53.6961
     22          79       2.7104    -0.9085       0.4180          -71.7688              33.0189
     23         103       2.8336    -0.9529       0.3032          -98.1530              31.2247
     24          65       2.9568    -0.9830       0.1837          -63.8933              11.9437
     25          51       3.0800    -0.9981       0.0616          -50.9033               3.1396
     26          76       3.2032    -0.9981      -0.0616          -75.8559              -4.6786
     27          9        3.3264    -0.9830      -0.1837           -8.8468              -1.6537
     28          46       3.4496    -0.9529      -0.3032          -43.8353             -13.9450
     29          27       3.5728    -0.9085      -0.4180          -24.5286             -11.2849
     30          16       3.6960    -0.8502      -0.5264          -13.6035              -8.4229
     31          11       3.8192    -0.7791      -0.6269           -8.5699              -6.8962
     32          11       3.9424    -0.6961      -0.7179           -7.6575              -7.8970
     33          0        4.0656    -0.6026      -0.7980            0.0000               0.0000
     34          11       4.1888    -0.5000      -0.8660           -5.5000              -9.5263
     35          0        4.3120    -0.3898      -0.9209            0.0000               0.0000
     36          0        4.4352    -0.2737      -0.9618            0.0000               0.0000
     37          42       4.5584    -0.1534      -0.9882           -6.4424             -41.5029
     38          56       4.6816    -0.0308      -0.9995           -1.7245             -55.9734
     39          32       4.8048     0.0923      -0.9957            2.9526             -31.8635
     40          48       4.9280     0.2139      -0.9768           10.2688             -46.8887
     41          40       5.0512     0.3324      -0.9432           13.2942             -37.7262
     42          0        5.1744     0.4457      -0.8952            0.0000               0.0000
     43          0        5.2976     0.5524      -0.8336            0.0000               0.0000
     44          0        5.4208     0.6506      -0.7594            0.0000               0.0000
     45          0        5.5440     0.7390      -0.6737            0.0000               0.0000
     46          0        5.6672     0.8162      -0.5778            0.0000               0.0000
     47          0        5.7904     0.8810      -0.4731            0.0000               0.0000
     48          0        5.9136     0.9325      -0.3612            0.0000               0.0000
     49          0        6.0368     0.9698      -0.2439            0.0000               0.0000
     50          0        6.1600     0.9924      -0.1229            0.0000               0.0000
     51          0        6.2832     1.0000       0.0000            0.0000               0.0000
   TOTAL        8205                0.0000       0.0000         2065.2801            5521.8088



                                                 8
Table 1 shows that the calculations for Fourier series by using Excel. From the table, we
can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is
25.5 which is half of 51 (numbers of data).

              1 51
       a0       yk
              L k 1
             8205
           
               51
            160.8824


             51          nx  
              y k  cos
                                
                                  
             k 1        L  
       a1 
                       L
            2605.2801
          
                  25.5
           80.9914


             51           nx  
              y k  sin 
                                 
                                   
             k 1         L  
       b1 
                       L
            5521.808
          
                 25.5
           216.5415


Then, we arrange the Fourier series as follow:

                   160.8824                x                  x 
        f ( x)              80.9914 cos       216.5415 sin        ...
                       2                  25.5                25.5 




                                                9
We can write the sum of sine and cosine term, with the same periodic which focus on the
first harmonic by calculated the value of c0, c1 and α1.

             a0
        c0 
              2
             160.8824
           
                 2
            80.4412



        c1  a12  b12 ,
            80.9914 2  216.5415 2
            231.1922


                     a1 
         1  tan 1 
                        
                         
                     b1 
                     80.9914 
            tan 1           
                     216.5415 
            0.3579
Then,
                                   x         
        y  80.4412  231.1922 sin            
                                   L  0.3579 
                                              

This equation is plotted by using Maple software to determine the peak value and analyze
the trend of dengue cases.




                                          10
>
>


>

      Figure 3. Fourier series graph plotted for dengue cases in Shah Alam (2009)




Figure 3 shows the Fourier series plotted with Maple software in first harmonic. The y-
axis represents the number of dengue cases and the x-axis represents the number of
weeks. From the graph, it shows that the maximum point or peak point in week 10 with
310 dengue cases. However, between week 26 to week 45, the graph shows that the
minimum number of case which is zero. It happened because the different or gap
between actual data for maximum cases and minimum cases is high. Early hypothesis
from this graph is the highest cases happen in week 10 with 310 cases and the lowest
cases happen between week 26 to week 45.




                                          11
Table 2. Fourier series calculation by using excel for dengue cases in Gombak (2009)
Week (x)   Cases (y)   (πx)/L   cos [(πx)/L]   sin [(πx)/L ]   [cos [(πx)/L]]*yk   [[sin (πx/L)] *yk]
   1         257       0.1232      0.9924          0.1229          255.0521              31.5823
   2         217       0.2464      0.9698          0.2439          210.4459              52.9293
   3         158       0.3696      0.9325          0.3612          147.3306              57.0762
   4         118       0.4928      0.8810          0.4731          103.9594              55.8250
   5         136       0.6160      0.8162          0.5778          111.0028              78.5772
   6         142       0.7392      0.7390          0.6737          104.9393              95.6648
   7         190       0.8624      0.6506          0.7594          123.6175             144.2869
   8          80       0.9856      0.5524          0.8336           44.1892              66.6882
   9         274       1.1088      0.4457          0.8952          122.1323             245.2747
  10         269       1.2320      0.3324          0.9432           89.4034             253.7085
  11         362       1.3552      0.2139          0.9768           77.4438             353.6191
  12         364       1.4784      0.0923          0.9957           33.5857             362.4472
  13         381       1.6016     -0.0308          0.9995          -11.7329             380.8193
  14         267       1.7248     -0.1534          0.9882          -40.9556             263.8402
  15         256       1.8480     -0.2737          0.9618          -70.0577             246.2274
  16         240       1.9712     -0.3898          0.9209          -93.5486             221.0173
  17          19       2.0944     -0.5000          0.8660           -9.5000              16.4545
  18         160       2.2176     -0.6026          0.7980          -96.4215             127.6828
  19          17       2.3408     -0.6961          0.7179          -11.8343              12.2045
  20          17       2.4640     -0.7791          0.6269          -13.2444              10.6577
  21          17       2.5872     -0.8502          0.5264          -14.4537               8.9493
  22          58       2.7104     -0.9085          0.4180          -52.6910              24.2417
  23          57       2.8336     -0.9529          0.3032          -54.3177              17.2797
  24          63       2.9568     -0.9830          0.1837          -61.9273              11.5762
  25          67       3.0800     -0.9981          0.0616          -66.8729               4.1246
  26          79       3.2032     -0.9981         -0.0616          -78.8502              -4.8633
  27          85       3.3264     -0.9830         -0.1837          -83.5527             -15.6187
  28         100       3.4496     -0.9529         -0.3032          -95.2942             -30.3153
  29         189       3.5728     -0.9085         -0.4180         -171.6999             -78.9945
  30         131       3.6960     -0.8502         -0.5264         -111.3784             -68.9626
  31         111       3.8192     -0.7791         -0.6269          -86.4779             -69.5885
  32         104       3.9424     -0.6961         -0.7179          -72.3979             -74.6628
  33          61       4.0656     -0.6026         -0.7980          -36.7607             -48.6791
  34          91       4.1888     -0.5000         -0.8660          -45.5000             -78.8083
  35          59       4.3120     -0.3898         -0.9209          -22.9974             -54.3334
  36          69       4.4352     -0.2737         -0.9618          -18.8827             -66.3660
  37          90       4.5584     -0.1534         -0.9882          -13.8052             -88.9349
  38          81       4.6816     -0.0308         -0.9995           -2.4944             -80.9616
  39          59       4.8048      0.0923         -0.9957            5.4438             -58.7483
  40          63       4.9280      0.2139         -0.9768           13.4778             -61.5414
  41         113       5.0512      0.3324         -0.9432           37.5561            -106.5765
  42          67       5.1744      0.4457         -0.8952           29.8645             -59.9759
  43         109       5.2976      0.5524         -0.8336           60.2078             -90.8627
  44          51       5.4208      0.6506         -0.7594           33.1815             -38.7297
  45          42       5.5440      0.7390         -0.6737           31.0384             -28.2952
  46          65       5.6672      0.8162         -0.5778           53.0528             -37.5553
  47          53       5.7904      0.8810         -0.4731           46.6936             -25.0740
  48          50       5.9136      0.9325         -0.3612           46.6236             -18.0621
  49          20       6.0368      0.9698         -0.2439           19.3959              -4.8783
  50          22       6.1600      0.9924         -0.1229           21.8333              -2.7035
  51          14       6.2832      1.0000          0.0000           14.0000               0.0000
TOTAL        6164                 0.0000          0.0000           397.8217            1848.6629




                                               12
Table 2 shows that the calculations for Fourier series by using excel. From the table, we
can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is
25.5 which is half of 51 (numbers of data).

              1 51
       a0       yk
              L k 1
             6164
           
               51
            120.8627


             51          nx  
              y k  cos
                                
                                  
             k 1        L  
       a1 
                       L
            397.8217
          
                 25.5
           15.6009


             51           nx  
              y k  sin 
                                 
                                   
             k 1         L  
       b1 
                       L
            1848.6629
          
                  25.5
           72.4966


Then, we arrange the Fourier series as follow:

                   120.8627               x                 x 
        f ( x)             15.6009 cos       72.4966 sin        ...
                       2                 25.5               25.5 




                                               13
We can write the sum of sine and cosine term, with the same periodic which focus on the
first harmonic by calculated the value of c0, c1 and α1.

             a0
        c0 
              2
             120.8627
           
                 2
            60.4314



        c1  a12  b12 ,
            15.6009 2  72.4966 2
            74.1562


                     a1 
         1  tan 1 
                        
                         
                     b1 
                     15.6009 
            tan 1          
                     72.4966 
            0.2120
Then,
                                  x         
        y  60.4314  74.1562 sin            
                                  L  0.2120 
                                             

This equation is plotted by using Maple software to determine the peak value and analyze
the trend of dengue cases.




                                          14
>
>


>

        Figure 4. Fourier series graph plotted for dengue cases in Gombak (2009)




Figure 4 shows that Fourier series plotted with Maple software in first harmonic. The y-
axis represents the number of dengue cases and the x-axis represents the number of
weeks. From the graph, it shows that the maximum point or peak point in week 10 with
134 dengue cases. However, from week 32 to week 42, the graph shows that the
minimum number of case which is zero. It happened because the different or gap
between actual data for maximum cases and minimum cases is high. Early hypothesis
from this graph is the highest cases happen in week 10 with 134 cases and the lowest
cases happen between week 32 to week 42.




                                          15
Table 3. Fourier series calculations by using excel for dengue cases in Klang (2009)
 Week(x)   Cases (y)   (πx)/L   cos (πx/L)   sin (πx/L)   [cos ((πx)/L )]*yk   [sin ((πx)/L)] *yk
    1         0        0.1232     0.9924       0.1229            0.0000               0.0000
    2        116       0.2464     0.9698       0.2439          112.4964             28.2940
    3         41       0.3696     0.9325       0.3612           38.2314             14.8109
    4         64       0.4928     0.8810       0.4731           56.3848             30.2780
    5         0        0.6160     0.8162       0.5778            0.0000               0.0000
    6         22       0.7392     0.7390       0.6737           16.2582             14.8213
    7         37       0.8624     0.6506       0.7594           24.0729             28.0980
    8         49       0.9856     0.5524       0.8336           27.0659             40.8465
    9         84       1.1088     0.4457       0.8952           37.4420             75.1937
   10         78       1.2320     0.3324       0.9432           25.9237             73.5660
   11        145       1.3552     0.2139       0.9768           31.0203            141.6430
   12        189       1.4784     0.0923       0.9957           17.4387            188.1938
   13        178       1.6016    -0.0308       0.9995           -5.4815            177.9156
   14        210       1.7248    -0.1534       0.9882          -32.2122            207.5147
   15        236       1.8480    -0.2737       0.9618          -64.5845            226.9909
   16        334       1.9712    -0.3898       0.9209         -130.1885            307.5824
   17        125       2.0944    -0.5000       0.8660          -62.5000            108.2532
   18        178       2.2176    -0.6026       0.7980         -107.2690            142.0471
   19        130       2.3408    -0.6961       0.7179          -90.4974             93.3285
   20        109       2.4640    -0.7791       0.6269          -84.9198             68.3347
   21         89       2.5872    -0.8502       0.5264          -75.6693             46.8525
   22         60       2.7104    -0.9085       0.4180          -54.5079             25.0776
   23         48       2.8336    -0.9529       0.3032          -45.7412             14.5513
   24         20       2.9568    -0.9830       0.1837          -19.6595               3.6750
   25         9        3.0800    -0.9981       0.0616           -8.9829               0.5540
   26         9        3.2032    -0.9981      -0.0616           -8.9829              -0.5540
   27         4        3.3264    -0.9830      -0.1837           -3.9319              -0.7350
   28         6        3.4496    -0.9529      -0.3032           -5.7177              -1.8189
   29         6        3.5728    -0.9085      -0.4180           -5.4508              -2.5078
   30         0        3.6960    -0.8502      -0.5264            0.0000               0.0000
   31         0        3.8192    -0.7791      -0.6269            0.0000               0.0000
   32         0        3.9424    -0.6961      -0.7179            0.0000               0.0000
   33         2        4.0656    -0.6026      -0.7980           -1.2053              -1.5960
   34         0        4.1888    -0.5000      -0.8660            0.0000               0.0000
   35         0        4.3120    -0.3898      -0.9209            0.0000               0.0000
   36         0        4.4352    -0.2737      -0.9618            0.0000               0.0000
   37         8        4.5584    -0.1534      -0.9882           -1.2271              -7.9053
   38         0        4.6816    -0.0308      -0.9995            0.0000               0.0000
   39         0        4.8048     0.0923      -0.9957            0.0000               0.0000
   40         0        4.9280     0.2139      -0.9768            0.0000               0.0000
   41         0        5.0512     0.3324      -0.9432            0.0000               0.0000
   42         0        5.1744     0.4457      -0.8952            0.0000               0.0000
   43         0        5.2976     0.5524      -0.8336            0.0000               0.0000
   44         0        5.4208     0.6506      -0.7594            0.0000               0.0000
   45         0        5.5440     0.7390      -0.6737            0.0000               0.0000
   46         0        5.6672     0.8162      -0.5778            0.0000               0.0000
   47         0        5.7904     0.8810      -0.4731            0.0000               0.0000
   48         0        5.9136     0.9325      -0.3612            0.0000               0.0000
   49         16       6.0368     0.9698      -0.2439           15.5168              -3.9026
   50         8        6.1600     0.9924      -0.1229            7.9394              -0.9831
   51         0        6.2832     1.0000       0.0000            0.0000               0.0000
 TOTAL      2610                  0.0000       0.0000         -398.9390            2038.4200



                                              16
Table 3 shows that the calculations for Fourier series by using excel. From the table, we
can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is
25.5 which is half of 51 (numbers of data).

             1 51
       a0      yk
             L k 1
             2610
           
              51
            51.1765


             51          nx  
              y k  cos
                                
                                  
             k 1        L  
       a1 
                       L
             398.9390
          
                  25.5
           15.6447


             51           nx  
              y k  sin 
                                 
                                   
             k 1         L  
       b1 
                       L
            2038.4200
          
                  25.5
           79.9380


Then, we arrange the Fourier series as follow:

                   51.1765                  x                 x 
        f ( x)              15.6447 cos       79.9380 sin        ...
                      2                    25.5               25.5 




                                                17
We can write the sum of sine and cosine term, with the same periodic which focus on the
first harmonic by calculated the value of c0, c1 and α1.

             a0
        c0 
              2
             51.1765
           
                2
            25.5882



        c1  a12  b12 ,
            (15.6447) 2  (79.9380) 2
            81.4546


                     a1 
         1  tan 1 
                        
                         
                     b1 
                      15.6447 
            tan 1            
                     79.9380 
            0.1933
Then,
                                  x          
        y  25.5882  81.4546 sin
                                  L   0.1933 
                                               
                                              

This equation is plotted by using Maple software to determine the peak value and analyze
the trend of dengue cases.




                                          18
>
>


>


         Figure 5. Fourier series graph plotted for dengue cases in Klang (2009)




Figure 5 shows that Fourier series that plotted with Maple software in first harmonic. For
y-axis represents the number of dengue cases and for x-axis represents the number of
weeks. From the graph, it shows that the maximum point or peak point in week 15 with
120 dengue cases. However, from week 30 to week 50, the graph shows that the
minimum number of case which is zero. It happened because the different or gap
between actual data for maximum cases and minimum cases is high. Early hypothesis
from this graph is the highest cases happen in week 15 with 120 cases and the lowest
cases happen between weeks 30 to week 50.




                                           19
Table 4. Fourier series calculations for dengue cases in Shah Alam (2010)

Week (x) Total (y) (πx)/L cos [(πx)/L] sin [(πx)/L] cos [(πx)/L] *Yk sin [(πx)/L] *Yk
   1         56     0.2027      0.9795       0.2013           54.8537            11.2727
   2         77     0.4054      0.9190       0.3944           70.7598            30.3654
   3         85     0.6081      0.8208       0.5713           69.7649            48.5578
   4        140     0.8107      0.6890       0.7248           96.4554           101.4710
   5        168     1.0134      0.5290       0.8486           88.8660           142.5722
   6        172     1.2161      0.3473       0.9378           59.7365           161.2934
   7        168     1.4188      0.1514       0.9885           25.4399           166.0627
   8        166     1.6215     -0.0506       0.9987           -8.4078           165.7869
   9        162     1.8242     -0.2507       0.9681          -40.6057           156.8285
  10        119     2.0268     -0.4404       0.8978          -52.4069           106.8387
  11        109     2.2295     -0.6121       0.7908          -66.7196            86.1946
  12        110     2.4322     -0.7588       0.6514          -83.4634            71.6510
  13         61     2.6349     -0.8743       0.4853          -53.3351            29.6034
  14         82     2.8376     -0.9541       0.2994          -78.2394            24.5478
  15         74     3.0403     -0.9949       0.1012          -73.6203             7.4865
  16         69     3.2429     -0.9949       -0.1012         -68.6460            -6.9806
  17         44     3.4456     -0.9541       -0.2994         -41.9821           -13.1720
  18         41     3.6483     -0.8743       -0.4853         -35.8482           -19.8974
  19         14     3.8510     -0.7588       -0.6514         -10.6226            -9.1192
  20         14     4.0537     -0.6121       -0.7908          -8.5695           -11.0709
  21         10     4.2564     -0.4404       -0.8978          -4.4039            -8.9780
  22         13     4.4590     -0.2507       -0.9681          -3.2585           -12.5850
  23          5     4.6617     -0.0506       -0.9987          -0.2532            -4.9936
  24          6     4.8644      0.1514       -0.9885           0.9086            -5.9308
  25         22     5.0671      0.3473       -0.9378           7.6407           -20.6305
  26         29     5.2698      0.5290       -0.8486          15.3400           -24.6107
  27         34     5.4725      0.6890       -0.7248          23.4249           -24.6430
  28         27     5.6751      0.8208       -0.5713          22.1606           -15.4242
  29         21     5.8778      0.9190       -0.3944          19.2981            -8.2815
  30         29     6.0805      0.9795       -0.2013          28.4064            -5.8377
  31         23     6.2832      1.0000       0.0000           23.0000             0.0000
TOTAL      2150                 0.0000       0.0000          -24.3271          1118.3775




                                            20
Table 4 shows that the calculations for Fourier series by using excel. From the table, we
can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is
15.5 which is half of 31 (numbers of data).

             1 31
       a0      yk
             L k 1
             2150
           
              31
            69.3548


             31          nx  
              y k  cos
                                
                                  
             k 1        L  
       a1 
                       L
             24.3271
          
                 15.5
           1.5695


             31           nx  
              y k  sin 
                                 
                                   
             k 1         L  
       b1 
                       L
            1118.3775
          
                 15.5
           72.1534


Then, we arrange the Fourier series as follow:

                   69.3548                 x                 x 
        f ( x)              1.5695 cos       72.1534 sin        ...
                      2                   15.5               15.5 




                                                21
We can write the sum of sine and cosine term, with the same periodic which focus on the
first harmonic by calculated the value of c0, c1 and α1.

             a0
        c0 
              2
             69.3548
           
                2
            34.6774



        c1  a12  b12 ,
            (1.5695) 2  (72.1534) 2
            72.1705


                     a1 
         1  tan 1 
                        
                         
                     b1 
                      1.5695 
            tan 1           
                     72.1534 
            0.0217
Then,
                                  x          
        y  34.6774  72.1705 sin
                                  L   0.0217 
                                               
                                              

This equation is plotted by using Maple software to determine the peak value and analyze
the trend of dengue cases.




                                          22
>
>


>

       Figure 6. Fourier series graph plotted for dengue cases in Shah Alam (2010)




Figure 6 shows that Fourier series that plotted with Maple software in first harmonic. The
y-axis represents the number of dengue cases and the x-axis represents the number of
weeks. From the graph, it shows that the maximum point or peak point in week 9 with
120 dengue cases. However, from week 18 to week 28, the graph shows that the
minimum number of case which is zero. It happened because the different or gap
between actual data for maximum cases and minimum cases is high. Early hypothesis
from this graph is the highest cases happen in week 9 with 120 cases and the lowest cases
happen between week 18 to week 28.




                                           23
Table 5. Fourier series calculations by using excel for dengue cases in Gombak (2010)
Week (x) Cases (y) (πx)/L cos [(πx)/L] sin [(πx)/L] [cos [(πx)/L]]*yk [sin [(πx)/L]] *yk
   1         118      0.2027       0.9795        0.2013           115.5845           23.7532
   2         126      0.4054       0.9190        0.3944           115.7887           49.6888
   3         117      0.6081       0.8208        0.5713            96.0293           66.8384
   4         184      0.8107       0.6890        0.7248           126.7699         133.3619
   5         185      1.0134       0.5290        0.8486            97.8583         156.9992
   6         184      1.2161       0.3473        0.9378            63.9042         172.5464
   7         183      1.4188       0.1514        0.9885            27.7113         180.8897
   8         174      1.6215      -0.0506        0.9987            -8.8130         173.7767
   9         192      1.8242      -0.2507        0.9681           -48.1253         185.8708
  10         180      2.0268      -0.4404        0.8978           -79.2709         161.6048
  11         188      2.2295      -0.6121        0.7908          -115.0759         148.6658
  12         166      2.4322      -0.7588        0.6514          -125.9538         108.1278
  13         100      2.6349      -0.8743        0.4853           -87.4347           48.5302
  14         125      2.8376      -0.9541        0.2994          -119.2674           37.4204
  15          77      3.0403      -0.9949        0.1012           -76.6049            7.7900
  16          92      3.2429      -0.9949        -0.1012          -91.5280           -9.3075
  17          74      3.4456      -0.9541        -0.2994          -70.6063          -22.1529
  18          67      3.6483      -0.8743        -0.4853          -58.5812          -32.5152
  19          58      3.8510      -0.7588        -0.6514          -44.0080          -37.7796
  20          52      4.0537      -0.6121        -0.7908          -31.8295          -41.1203
  21          46      4.2564      -0.4404        -0.8978          -20.2581          -41.2990
  22          46      4.4590      -0.2507        -0.9681          -11.5300          -44.5315
  23          54      4.6617      -0.0506        -0.9987           -2.7351          -53.9307
  24          55      4.8644       0.1514        -0.9885            8.3285          -54.3658
  25          66      5.0671       0.3473        -0.9378           22.9221          -61.8916
  26          67      5.2698       0.5290        -0.8486           35.4406          -56.8592
  27          86      5.4725       0.6890        -0.7248           59.2512          -62.3322
  28         109      5.6751       0.8208        -0.5713           89.4632          -62.2682
  29         130      5.8778       0.9190        -0.3944          119.4645          -51.2663
  30         138      6.0805       0.9795        -0.2013          135.1751          -27.7792
  31         132      6.2832       1.0000        0.0000           132.0000            0.0000
TOTAL       3571                   0.0000        0.0000           254.0694         996.4649




                                            24
Table 5 shows that the calculations for Fourier series by using excel. From the table, we
can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is
15.5 which is half of 31 (numbers of data).

              1 31
       a0       yk
              L k 1
             3571
           
               31
            115.1935


             31          nx  
              y k  cos
                                
                                  
             k 1        L  
       a1 
                       L
            254.0694
          
                 15.5
           16.3916


             31           nx  
              y k  sin 
                                 
                                   
             k 1         L  
       b1 
                       L
            996.4649
          
                 15.5
           64.2881


Then, we arrange the Fourier series as follow:

                   115.1935              x                x 
        f ( x)             16.3981cos       64.2881sin        ...
                       2                15.5              15.5 




                                               25
We can write the sum of sine and cosine term, with the same periodic which focus on the
first harmonic by calculated the value of c0, c1 and α1.

             a0
        c0 
              2
             115.1935
           
                 2
            57.5968



        c1  a12  b12 ,
            (16.3916) 2  (64.2881) 2
            66.3448


                     a1 
         1  tan 1 
                        
                         
                     b1 
                     16.3916 
            tan 1          
                     64.2881 
            0.2497
Then,
                                  x          
        y  57.5968  66.3448 sin
                                  L   0.2497 
                                               
                                              

This equation is plotted by using Maple software to determine the peak value and analyze
the trend of dengue cases.




                                          26
>
>


>

        Figure 7. Fourier series graph plotted for dengue cases in Gombak (2010)




Figure 7 shows that Fourier series that plotted with Maple software in first harmonic. The
y-axis represents the number of dengue cases and the x-axis represents the number of
weeks. From the graph, it shows that the maximum point or peak point in week 7 with
120 dengue cases. However, from week 19 to week 24, the graph shows that the
minimum number of case which is zero. It happened because the different or gap
between actual data for maximum cases and minimum cases is high. Early hypothesis
from this graph is the highest cases happen in week 7 with 120 cases and the lowest cases
happen between week 19 to week 24.




                                           27
Table 6. Fourier series calculations by using excel for dengue cases in Klang (2010)

Week(x) Total (y) (πx)/L cos (πx)/L sin (πx)/L [cos [(πx)/L]] *yk [sin [(πx)/L]] *yk
   1         20      0.2027      0.9795      0.2013          19.5906               4.0260
   2         14      0.4054      0.9190      0.3944          12.8654               5.5210
   3         17      0.6081      0.8208      0.5713          13.9530               9.7116
   4         40      0.8107      0.6890      0.7248          27.5587              28.9917
   5         48      1.0134      0.5290      0.8486          25.3903              40.7349
   6         47      1.2161      0.3473      0.9378          16.3233              44.0744
   7         53      1.4188      0.1514      0.9885           8.0257              52.3888
   8         59      1.6215     -0.0506      0.9987           -2.9883             58.9243
   9         43      1.8242     -0.2507      0.9681          -10.7781             41.6273
  10         53      2.0268     -0.4404      0.8978          -23.3409             47.5836
  11         51      2.2295     -0.6121      0.7908          -31.2174             40.3296
  12         47      2.4322     -0.7588      0.6514          -35.6616             30.6145
  13         38      2.6349     -0.8743      0.4853          -33.2252             18.4415
  14         41      2.8376     -0.9541      0.2994          -39.1197             12.2739
  15         50      3.0403     -0.9949      0.1012          -49.7435              5.0584
  16         53      3.2429     -0.9949     -0.1012          -52.7281             -5.3619
  17         20      3.4456     -0.9541     -0.2994          -19.0828             -5.9873
  18         25      3.6483     -0.8743     -0.4853          -21.8587            -12.1325
  19         29      3.8510     -0.7588     -0.6514          -22.0040            -18.8898
  20         24      4.0537     -0.6121     -0.7908          -14.6905            -18.9786
  21         21      4.2564     -0.4404     -0.8978           -9.2483            -18.8539
  22         12      4.4590     -0.2507     -0.9681           -3.0078            -11.6169
  23         13      4.6617     -0.0506     -0.9987           -0.6584            -12.9833
  24         14      4.8644      0.1514     -0.9885           2.1200             -13.8386
  25         15      5.0671      0.3473     -0.9378           5.2096             -14.0663
  26         19      5.2698      0.5290     -0.8486          10.0503             -16.1242
  27         15      5.4725      0.6890     -0.7248          10.3345             -10.8719
  28         16      5.6751      0.8208     -0.5713          13.1322              -9.1403
  29         13      5.8778      0.9190     -0.3944          11.9465              -5.1266
  30         31      6.0805      0.9795     -0.2013          30.3654              -6.2403
  31         33      6.2832      1.0000      0.0000          33.0000               0.0000
TOTAL       974                  0.0000      0.0000         -129.4878            260.0890




                                             28
Table 6 shows that the calculations for Fourier series by using excel. From the table, we
can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is
15.5 which is half of 31 (numbers of data).

             1 31
       a0      yk
             L k 1
             974
           
              31
            31.4194


             31          nx  
              y k  cos
                                
                                  
             k 1        L  
       a1 
                       L
             129.4878
          
                  15.5
           8.3541


             31           nx  
              y k  sin 
                                 
                                   
             k 1         L  
       b1 
                       L
            260.0890
          
                 15.5
           16.7799


Then, we arrange the Fourier series as follow:

                   31.4194                x                 x 
        f ( x)              8.3541cos       16.7799 sin        ...
                      2                  15.5               15.5 




                                                29
We can write the sum of sine and cosine term, with the same periodic which focus on the
first harmonic by calculated the value of c0, c1 and α1.

             a0
        c0 
              2
             31.4194
           
                 2
            15.7097



        c1  a12  b12 ,
            (8.3541) 2  (16.7799) 2
            18.7445


                     a1 
         1  tan 1 
                        
                         
                     b1 
                      8.3541 
            tan 1           
                     16.7799 
            0.4619
Then,
                                  x          
        y  15.7097  18.7445 sin
                                  L   0.4619 
                                               
                                              

This equation is plotted by using Maple software to determine the peak value and analyze
the trend of dengue cases.




                                           30
>
>


>

         Figure 8. Fourier series graph plotted for dengue cases in Klang (2010)




Figure 8 shows that Fourier series that plotted with Maple software in first harmonic. The
y-axis represents the number of dengue cases and the x-axis represents the number of
weeks. From the graph, it shows that the maximum point or peak point in week 10 with
35 dengue cases. However, from week 23 to week 28, the graph shows that the minimum
number of case which is zero. It happened because the different or gap between actual
data for maximum cases and minimum cases is high. Early hypothesis from this graph is
the highest cases happen in week 10 with 35 cases and the lowest cases happen between
week 23 to week 28.




                                           31
4.     RESULTS AND DISCUSSION

From the findings, it can be noticed that the data of dengue cases in these three districts
which are Shah Alam, Gombak and Klang is distributed fluctuation. It is difficult to
determine and predict the dengue cases for the next year by following the trend line that is
generated by Excel.

                Table 7. Fourier series equations on 1st harmonic for 2009
                District                Fourier Series Equation

              Shah Alam y= 80.4412 + 231.1922sin[(πx/25.5) + 0.3579]
               Gombak   y= 60.4314 + 74.1562 sin[(πx/25.5) + 0.2120]
                Klang    y= 25.5882 + 81.4546 sin[(πx/25.5) -0.1933]



                Table 8. Fourier series equations on 1st harmonic for 2010
                 District               Fourier Series Equation

               Shah Alam y= 34.6774 + 72.1705sin [(πx/15.5) – 0.0217]
                Gombak    y= 57.5968 + 66.344sin [(πx/15.5) +0.2497]
                 Klang   y= 15.7097 + 18.7445sin [(πx/15.5) – 0.4619]



               Table 9. Analysis from graph using maple software for 2009
                             District   Peak Value Cases Week

                            Shah Alam         310            10
                             Gombak           130            10
                              Klang           110            12



              Table 10. Analysis from graph using maple software for 2010
                             District   Peak Value Cases Week

                            Shah Alam         120             9
                             Gombak           120             7
                              Klang            35            10




                                            32
The equation of Fourier series on first harmonic for dengue cases are shown in Table 7
and Table 8. For the year 2009, dengue cases seasonally peak between period week 10 to
14 (14 March 2009 until 11 April 2009) averagely recorded between 100 and 300 cases
per week. It also shows that dengue cases dengue cases slowly decrease for chosen
district at the end of year 2009. For the year 2010, dengue cases seasonally peak between
period week 7 to week 10 (20 February 2010 until 13 March 2010) averagely recorded
between 35 and 120 cases per week. It also shows that dengue cases dengue cases slowly
decrease for chosen district started from week 18 to week 28 (8 May 2010 to 18 July).

If we want to compare the result between year 2009 and 2010, we can see dengue cases
seasonally peak at first quarter of year which averagely recorded in period week 7 to
week 14 (February to April). Then, the dengue cases will reduce slowly in the third
quarter of the year.


5.     CONCLUSIONS AND RECOMMENDATIONS

Dengue is one of the diseases with no specific treatment or immunizations. Thus, the
preventive precautions from dengue such as fogging are important to reduce the cases.

We can summarize that the peak dengue cases is peak between first quarter of the year
which averagely recorded in period week 7 to week 14 (February to April). Shah Alam
recorded the highest dengue cases in 2009 which 310 cases in week 10 compared to
Klang which recorded 110. In year 2010, Shah Alam and Klang show drastic decrease the
number of cases which 120 and 35 cases respectively. However, Gombak did not record
the decrease cases in year 2010 compared to year 2009 which gives average of 120 cases.

From the findings, it is recommended that the Ministry of Health Malaysia should focus
more on first quarter of the year (February until April) every year to reduce dengue cases
because this period recorded highest cases in 2009 and 2010.

Further studies can be done for the previous year such as 2008 or 2007. So, the seasonal
peak can be determined further. This model can be explored further by comparing the
dengue cases recorded with climatic variability that is rainfalls, temperature and vapor
pressure in those selected districts in Selangor. Comparison can also be done between
states in Malaysia.




                                           33
REFERENCES

Abas N., Daud Z.M., Yusof F. (2009). Fourier Series In A Temporal Rainfall Model.
Proceeding of the 5th Asian Mathematical Conference, Malaysia.

Ang, K.C. & Li, Zi. (1999). Modeling The Spread of Dengue in Singapore, Division of
Mathematics, School of Sciences, Nanyang Technological University, Singapore.

Angove, C. (2009). Some Discrete Real And Complex Fourier Transforms, A Discussion,
With Examples.

Favier, C., Degallier, N. & Dubois, M.A. (2005). Dengue Epidemic Modelling: Stakes
and Pitfalls.

Klingenberg, L. (2005). Frequency Domain Using Excel. San Francisco State University
School of Engineering.

Kvernadze, G., Hagstrom, T., and Shapiro, H. (2000). Detecting the Singularities of a
Function of VP Class by its Integrated Fourier Series. Computers and Mathematics with
Applications, 39, 25-43.

McNeal, J. D. and Zeytuncu, Y. U. (2006). A note on rearrangement of Fourier
series. J. Math. Anal. Appl. 323 (2006) 1348–1353.

Nuraini, N., Soewono, E. & Sidarto, K.A. (2006). Mathematical Model of Dengue
Disease Transmission with Severe DHF Compartment, Bulletin of the Malaysian
Mathematical Sciences Society, 30, 143-157.

Pongsumpun, P. & Tang, I.M. (2001). A Realistic Age Structure Transmission Model for
Dengue Hemorrhagic Fever in Thailand, Department of Mathematics and Physics,
Faculty of Sciences, Mahidol University.

Tamrin, H., Riyanto, M.Z., Akhid Ardhian, A. (2007). Not Fatal Disease For SIR Model.

Zill, D.G. & Cullen, M. R. (2009). Differential Equations With Boundary-Value
Problems, 7th Edition, International Student Edition.




                                         34

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Technical Report (Comparison Of Dengue Cases For Chosen District In Selangor By Using Fourier Series)

  • 1. ACKNOWLEDGEMENTS IN THE NAME OF ALLAH, THE MOST GRACIOUS, THE MOST MERCIFUL Firstly, I am grateful to Allah S.W.T for giving me the strength to complete this project successfully. I would like to express my gratitude Associated Professor Maheran Nuruddin for the guidance and support to this report. Special thanks to my family, especially my parent who always support and pray for my success. I wish to thank my friends for their support. They have been very supportive throughout the completion of this project. Last but not least, thank you again for those who spent time and effort with me in completing this report, directly or indirectly. Without Allah bless and the all kindness of these people, I will never succeed in completing this project. Thank you so much. Wasalam.
  • 2. TABLE OF CONTENTS ACKNOWLEDGEMENTS ................................................................................................. i TABLE OF CONTENTS .................................................................................................... ii LIST OF TABLES ............................................................................................................. iii LIST OF FIGURES ........................................................................................................... iii ABSTRACT ....................................................................................................................... iv 1. INTRODUCTION ........................................................................................................ 1 2. METHODOLOGY ....................................................................................................... 4 3. IMPLEMENTATION ................................................................................................... 6 4. RESULTS AND DISCUSSION ................................................................................. 32 5. CONCLUSIONS AND RECOMMENDATIONS ..................................................... 33 REFERENCES ................................................................................................................. 34 ii
  • 3. LIST OF TABLES Table 1. Fourier series calculation by using excel for dengue cases in Shah Alam (2009) . 8 Table 2. Fourier series calculation by using excel for dengue cases in Gombak (2009) ... 12 Table 3. Fourier series calculations by using excel for dengue cases in Klang (2009) ..... 16 Table 4. Fourier series calculations for dengue cases in Shah Alam (2010) ..................... 20 Table 5. Fourier series calculations by using excel for dengue cases in Gombak (2010) . 24 Table 6. Fourier series calculations by using excel for dengue cases in Klang (2010) ..... 28 Table 7. Fourier series equations on 1st harmonic for 2009 .............................................. 32 Table 8. Fourier series equations on 1st harmonic for 2010 .............................................. 32 Table 9. Analysis from graph using maple software for 2009 ........................................... 32 Table 10. Analysis from graph using maple software for 2010 ......................................... 32 LIST OF FIGURES Figure 1. Graph of dengue cases in Shah Alam, Gombak and Klang for year 2009 ........... 6 Figure 2. Graph of dengue cases in Shah Alam, Gombak and Klang for year 2010 ........... 7 Figure 3. Fourier series graph plotted for dengue cases in Shah Alam (2009) .................. 11 Figure 4. Fourier series graph plotted for dengue cases in Gombak (2009) ...................... 15 Figure 5. Fourier series graph plotted for dengue cases in Klang (2009) .......................... 19 Figure 6. Fourier series graph plotted for dengue cases in Shah Alam (2010) .................. 23 Figure 7. Fourier series graph plotted for dengue cases in Gombak (2010) ...................... 27 Figure 8. Fourier series graph plotted for dengue cases in Klang (2010) .......................... 31 iii
  • 4. ABSTRACT Dengue is the most dangerous mosquito virus infection to the human in the world. Up to 100 million cases are reported annually and some two billion people are at risk of infection in the world. There is no specific cure or medicine to shorten the course of dengue. The occurrence of dengue in Malaysia has become more serious year to year. The aims of this study are to know the pattern of dengue cases that happened in chosen district and to obtain the highest point for dengue cases in chosen district by referring to Fourier series graph plotted. This project focuses on certain districts which had recorded the highest dengue cases among district in Malaysia which are Shah Alam, Gombak and Klang. It is difficult to determine and predict the dengue cases for the next year by following the trend line that is generated by Excel. Thus, the alternative that we have is to transform the graph into a periodic graph using Fourier series, so that the highest point for the dengue cases can be determined. Fourier series is an expansion of a periodic function of period which the base is the set of sine functions. Hence, Fourier series is one of the alternative methods to compare and explain the pattern of dengue cases recorded. The result between year 2009 and 2010 show the number of dengue cases seasonally peak at first quarter of year which averagely recorded in period week 7 to week 14 (February to April). iv
  • 5. 1. INTRODUCTION Dengue is the most dangerous mosquito virus infection to the human in the world. Ang and Li (1999) stated that up to 100 million cases are reported annually and some two billion people are at risk of infection in the world. Dengue viruses are transmitted from vector (mosquitoes) to the susceptible human beings by various mosquitoes such as Aedes aegypti and Aedes albopictus. From that, the infected person will have a few symptoms such as high fever (40°C), chills, headache, pain in the eyes, deep muscle and joint pains and extreme fatigue. Actually, the infected person will have high fever for two to four days. Then, the body temperature will drop rapidly and intense sweating takes places. But, patient’s body will show up small red bumps. These are a few symptoms that will happen to the infected person. If the patient does not take immediately treatment, dengue may cause death. Knowing how dengue being transmitted is very important. This is relevant to this study because we must identify and know who is the vector and the host. Basically, dengue viruses are transmitted from the vector (mosquitoes) to the host (humans). The transmitted dengue virus process happened by mosquitoes bite during mosquitoes blood feeding. The mosquitoes also may carry the virus from one host to another host. When the virus has been transmitted to the host (humans) incubation period will occur. The dengue viruses multiply during incubation time. After three to five days, the symptoms of dengue will appear and attack patients. There is no specific cure or medicine to shorten the course of dengue. Actually, the medicine provided by doctors is to reduce and alleviate the symptoms and sign of dengue. In this situation, the patient (infected person) takes paracetamol to relieve muscle and joint aches, fever and headache. The patient is advice to keep rest in a screened room to prevent mosquitoes from entering. The dengue virus will be transmitted to another host (human) if the patient is bitten second times. After this treatment, in a few days, we can define the patient is fully recovered and in the best condition (recover person) when the symptoms had disappeared. The occurrence of dengue in Malaysia had become more serious year to year. The Ministry of Health Malaysia (2009) stated that dengue has become pandemic. Besides that, people did not take this problem as a serious problem. In order to increase the people’s sensitivity of dengue, the Ministry of Health has done many activities and campaign such as advertisement through the television and internet. The activities and campaign also include involvement of students in primary and secondary schools. For example, the competition “AntiAedes Ranjer Ridsect” organized by Sara Lee Company (Ridsect) which cooperated with Ministry of Health Malaysia. 1
  • 6. In order to analyze the dengue cases which happened in Malaysia for this study, Fourier series was choose because of its availability to present and show the new perspective analysis of dengue cases. Zill and Cullen (2009) stated that the representation of a function in the form of a series is widely and frequently used to solve and explain the common problem situation. The history of Fourier series started when Bernoulli, D’ Allembert and Euler (1750) had used and introduced the idea of expanding a function in the form a series to solve the associated with the vibration of strings. Then, Joseph Fourier who a French physicist, (1768-1830) improved and developed the approach of Fourier series where it was generally useful nowadays. However, the search had done by Joseph Fourier gave impact to all mathematicians and physicists at that time such as Laplace, Poisson and Lagrange. They doubt and debate about Fourier’s work because it opposite and inversed to their idea. But, the text of Joseph Forier which Theorie Analytique de la Chaleur (The Analytical Theory of Heat) become the source for the modern method in order to solve problems associated with partial differential equations subject to prescribed boundary conditions. Nowadays, the application of Fourier series analysis is commonly used in physic and electrical engineering sector which how frequency associated to a dynamical systems. The text from Joseph Fourier influenced in created electrical component such as electronic rectifiers. Fourier series also is the best method to analyze the data series such as dengue cases which useful to compare and determine the dengue cases happened in Malaysia. Angove (2009) analyze the periodic time domain voltage waveform and convert it to the frequency domain which always uses in electronic communication systems. For example a waveform usually decomposed into sum of harmonically related sine, cosine waveform and constant which is known as Fourier series. Klingenberg (2005) showed the way to apply and calculate Fourier series analysis by using Microsoft Excel. Excel generally shows the magnitude versus time is known waveform. Klingenberg (2005) done the experiments call for the “harmonic content” of a reproduced waveform is a display of the magnitude of the waveform (Y-axis) versus the frequency (X-axis). In other word, we called it as frequency spectrum and it allows visualizing a waveform according to its frequency content. Kvernadzi, Hagstrom and Shapiro (1999) studied about the utilization of the truncated Fourier series and it applies as a tool for the approximation of the points of discontinuities and the magnitudes by using integrals. Abas, Daud and Yusuf (2009) studied about rainfall by using Fourier series with significant number of harmonics is fitted to the model’s parameter. The results of their studies showed that statistical properties of the estimated rainfall series were able to match most of those of the historical series. The Fourier series makes the model more parsimony by grabs the seasonal fluctuations within the model. 2
  • 7. The strategy or plan must be systematic. So, modeling how dengue spread among population localized in a district guides the Ministry of Health Malaysia to prevent these epidemics become more danger to community. The model were showed the seasonal pattern that are useful in prevent in a spread of dengue. Favier (2006) suggest that, statistical analyses of longitudinal surveys sites are needed before choose the right parameters. The scope of this study was in small scale because Favier, Degallier and Dubois (2005) stated that possibility of transmission dengue also depends on the population density and previous immunization. Sometimes, factor likes rainfalls, temperature must be considered. The virus progression occurs at a daily scale; therefore it must be recorded in weeks or days to be more accurate and precise. So, the prediction and modeling of dengue repartition and dynamics raises must different depends on the situation and place. Since the scope of study is in small scale, the result will be more accurate. For instance, modeling of dengue prevalence is conceivable at town-scale like Shah Alam, Subang and Klang but not at global scale, where long-range interactions cannot model accurately. Dengue will impact high death rate if we are not able to control it. Being able to know the pattern and trend of dengue cases will be of great significant in reducing the death rate that will cause by dengue. A good and reliable mathematical modeling about pattern and trend dengue will help the government to take preventing control and precaution control to reduce the dengue case in certain time in the future since this disease does not have specific treatment. The objectives of this study are to know the pattern of dengue cases that happened in chosen district, to obtain the first harmonic equation of Fourier series and compare the peak value for dengue cases in the chosen district by referring to Fourier series graph plotted. This project focuses on certain districts which had recorded the highest dengue cases among district in Malaysia which are Shah Alam, Gombak and Klang. 3
  • 8. 2. METHODOLOGY Some of Fourier series formula from Zill and Cullen (2009) that are used throughout this study is given as follows:- The Fourier series of a function f defined on the interval [0, 2L] is given by: a   n n  f ( x)  0    a n cos x  bn sin x 2 n1  L L  where, 2L 1 a0  L  f ( x)dx 0 n 2L 1 an  L  f ( x) cos 0 L xdx n 2L 1 bn  L  f ( x) sin 0 L xdx Fourier series determined from the coefficient which are a0, an, and bn. Since, we are focus on the first harmonic term, we can write these coefficients as follow: 2L 1 a 0   f ( x)dx L 0 1    yk L k 1  y k  k 1 L  [average of f ( x)] n 2L 1 a1  L  f ( x) cos 0 L xdx 1   nx      y k  cos     L  k 1   L      nx     y k  cos      k 1   L    L 4
  • 9. n 2L 1 b1  L  f ( x) sin 0 L xdx 1   nx      y k  sin      L  k 1   L      nx     y k  sin       k 1   L    L where yk is data obtained from the dengue cases and 2L is the period time. Then, we arrange the Fourier series as follow: a  x x   2x 2x  f ( x)  0   a1 cos  b1 sin    a2 cos  b2 sin   ... 2  L L  L L   x x  The term of  a1 cos  b1 sin  is called the first harmonic. We can write the sum of  L L sine and cosine term, with the same periodic as follow:  x   2x  y  f ( x)  c0  c1 sin  1   c2 sin   2   ... L   L  where, a c0  0 , 2 c1  a12  b12 ,  a1   1  tan 1      b1  In this study, we focus on the first harmonic term on this equation which is:  x  y  c0  c1 sin  L  1     This equation is plotted by using Maple software to determine the peak value and analyze the trend of dengue cases. 5
  • 10. 3. IMPLEMENTATION Before proceed to Fourier series method, the data of dengue case were plotted by using Excel in order to look for the pattern of dengue cases which happened in Shah Alam, Gombak and Klang. Figure 1. Graph of dengue cases in Shah Alam, Gombak and Klang for year 2009 Figure1 shows that comparison of dengue cases between Shah Alam, Gombak and Klang since 7 January until 26 December 2009 by graph. From the graph above, it is hard to compare the pattern between these districts. Thus, it is not accurate if we want to generate the prediction for the next year based on the trend line equation. Furthermore, there are a lot of scatter plot dengue cases data that fluctuations over the period cover. 6
  • 11. Figure 2. Graph of dengue cases in Shah Alam, Gombak and Klang for year 2010 Figure2 shows that comparison of dengue cases between Shah Alam, Gombak and Klang since 9 January until 8 August 2010 by graph. From the graph above, it is hard to compare the pattern between these districts. Thus, it is not accurate if we want to generate the prediction for the next year based on the trend line equation. Furthermore, there are a lot of scatter plot dengue cases data that fluctuations over the period cover. So, more suitable method to compare the pattern of number of dengue cases recorded in Shah Alam, Gombak and Klang is Fourier series. 7
  • 12. Table 1. Fourier series calculation by using excel for dengue cases in Shah Alam (2009) Week (x) Cases (y) (πx)/L cos (πx/L) sin (πx/L) [cos ((πx)/L)] *yk [sin ((πx)/L)] *yk 1 244 0.1232 0.9924 0.1229 242.1506 29.9847 2 425 0.2464 0.9698 0.2439 412.1637 103.6633 3 362 0.3696 0.9325 0.3612 337.5549 130.7695 4 360 0.4928 0.8810 0.4731 317.1644 170.3137 5 474 0.6160 0.8162 0.5778 386.8773 273.8648 6 337 0.7392 0.7390 0.6737 249.0460 227.0354 7 525 0.8624 0.6506 0.7594 341.5746 398.6876 8 482 0.9856 0.5524 0.8336 266.2399 401.7963 9 489 1.1088 0.4457 0.8952 217.9661 437.7348 10 608 1.2320 0.3324 0.9432 202.0717 573.4379 11 521 1.3552 0.2139 0.9768 111.4591 508.9380 12 622 1.4784 0.0923 0.9957 57.3909 619.3467 13 552 1.6016 -0.0308 0.9995 -16.9989 551.7382 14 383 1.7248 -0.1534 0.9882 -58.7490 378.4674 15 260 1.8480 -0.2737 0.9618 -71.1524 250.0747 16 360 1.9712 -0.3898 0.9209 -140.3229 331.5260 17 41 2.0944 -0.5000 0.8660 -20.5000 35.5070 18 132 2.2176 -0.6026 0.7980 -79.5478 105.3383 19 127 2.3408 -0.6961 0.7179 -88.4090 91.1748 20 76 2.4640 -0.7791 0.6269 -59.2101 47.6462 21 102 2.5872 -0.8502 0.5264 -86.7221 53.6961 22 79 2.7104 -0.9085 0.4180 -71.7688 33.0189 23 103 2.8336 -0.9529 0.3032 -98.1530 31.2247 24 65 2.9568 -0.9830 0.1837 -63.8933 11.9437 25 51 3.0800 -0.9981 0.0616 -50.9033 3.1396 26 76 3.2032 -0.9981 -0.0616 -75.8559 -4.6786 27 9 3.3264 -0.9830 -0.1837 -8.8468 -1.6537 28 46 3.4496 -0.9529 -0.3032 -43.8353 -13.9450 29 27 3.5728 -0.9085 -0.4180 -24.5286 -11.2849 30 16 3.6960 -0.8502 -0.5264 -13.6035 -8.4229 31 11 3.8192 -0.7791 -0.6269 -8.5699 -6.8962 32 11 3.9424 -0.6961 -0.7179 -7.6575 -7.8970 33 0 4.0656 -0.6026 -0.7980 0.0000 0.0000 34 11 4.1888 -0.5000 -0.8660 -5.5000 -9.5263 35 0 4.3120 -0.3898 -0.9209 0.0000 0.0000 36 0 4.4352 -0.2737 -0.9618 0.0000 0.0000 37 42 4.5584 -0.1534 -0.9882 -6.4424 -41.5029 38 56 4.6816 -0.0308 -0.9995 -1.7245 -55.9734 39 32 4.8048 0.0923 -0.9957 2.9526 -31.8635 40 48 4.9280 0.2139 -0.9768 10.2688 -46.8887 41 40 5.0512 0.3324 -0.9432 13.2942 -37.7262 42 0 5.1744 0.4457 -0.8952 0.0000 0.0000 43 0 5.2976 0.5524 -0.8336 0.0000 0.0000 44 0 5.4208 0.6506 -0.7594 0.0000 0.0000 45 0 5.5440 0.7390 -0.6737 0.0000 0.0000 46 0 5.6672 0.8162 -0.5778 0.0000 0.0000 47 0 5.7904 0.8810 -0.4731 0.0000 0.0000 48 0 5.9136 0.9325 -0.3612 0.0000 0.0000 49 0 6.0368 0.9698 -0.2439 0.0000 0.0000 50 0 6.1600 0.9924 -0.1229 0.0000 0.0000 51 0 6.2832 1.0000 0.0000 0.0000 0.0000 TOTAL 8205 0.0000 0.0000 2065.2801 5521.8088 8
  • 13. Table 1 shows that the calculations for Fourier series by using Excel. From the table, we can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is 25.5 which is half of 51 (numbers of data). 1 51 a0   yk L k 1 8205  51  160.8824  51   nx     y k  cos      k 1   L   a1  L 2605.2801  25.5  80.9914  51   nx     y k  sin       k 1   L   b1  L 5521.808  25.5  216.5415 Then, we arrange the Fourier series as follow: 160.8824  x x  f ( x)    80.9914 cos  216.5415 sin   ... 2  25.5 25.5  9
  • 14. We can write the sum of sine and cosine term, with the same periodic which focus on the first harmonic by calculated the value of c0, c1 and α1. a0 c0  2 160.8824  2  80.4412 c1  a12  b12 ,  80.9914 2  216.5415 2  231.1922  a1   1  tan 1      b1   80.9914   tan 1    216.5415   0.3579 Then,  x  y  80.4412  231.1922 sin   L  0.3579    This equation is plotted by using Maple software to determine the peak value and analyze the trend of dengue cases. 10
  • 15. > > > Figure 3. Fourier series graph plotted for dengue cases in Shah Alam (2009) Figure 3 shows the Fourier series plotted with Maple software in first harmonic. The y- axis represents the number of dengue cases and the x-axis represents the number of weeks. From the graph, it shows that the maximum point or peak point in week 10 with 310 dengue cases. However, between week 26 to week 45, the graph shows that the minimum number of case which is zero. It happened because the different or gap between actual data for maximum cases and minimum cases is high. Early hypothesis from this graph is the highest cases happen in week 10 with 310 cases and the lowest cases happen between week 26 to week 45. 11
  • 16. Table 2. Fourier series calculation by using excel for dengue cases in Gombak (2009) Week (x) Cases (y) (πx)/L cos [(πx)/L] sin [(πx)/L ] [cos [(πx)/L]]*yk [[sin (πx/L)] *yk] 1 257 0.1232 0.9924 0.1229 255.0521 31.5823 2 217 0.2464 0.9698 0.2439 210.4459 52.9293 3 158 0.3696 0.9325 0.3612 147.3306 57.0762 4 118 0.4928 0.8810 0.4731 103.9594 55.8250 5 136 0.6160 0.8162 0.5778 111.0028 78.5772 6 142 0.7392 0.7390 0.6737 104.9393 95.6648 7 190 0.8624 0.6506 0.7594 123.6175 144.2869 8 80 0.9856 0.5524 0.8336 44.1892 66.6882 9 274 1.1088 0.4457 0.8952 122.1323 245.2747 10 269 1.2320 0.3324 0.9432 89.4034 253.7085 11 362 1.3552 0.2139 0.9768 77.4438 353.6191 12 364 1.4784 0.0923 0.9957 33.5857 362.4472 13 381 1.6016 -0.0308 0.9995 -11.7329 380.8193 14 267 1.7248 -0.1534 0.9882 -40.9556 263.8402 15 256 1.8480 -0.2737 0.9618 -70.0577 246.2274 16 240 1.9712 -0.3898 0.9209 -93.5486 221.0173 17 19 2.0944 -0.5000 0.8660 -9.5000 16.4545 18 160 2.2176 -0.6026 0.7980 -96.4215 127.6828 19 17 2.3408 -0.6961 0.7179 -11.8343 12.2045 20 17 2.4640 -0.7791 0.6269 -13.2444 10.6577 21 17 2.5872 -0.8502 0.5264 -14.4537 8.9493 22 58 2.7104 -0.9085 0.4180 -52.6910 24.2417 23 57 2.8336 -0.9529 0.3032 -54.3177 17.2797 24 63 2.9568 -0.9830 0.1837 -61.9273 11.5762 25 67 3.0800 -0.9981 0.0616 -66.8729 4.1246 26 79 3.2032 -0.9981 -0.0616 -78.8502 -4.8633 27 85 3.3264 -0.9830 -0.1837 -83.5527 -15.6187 28 100 3.4496 -0.9529 -0.3032 -95.2942 -30.3153 29 189 3.5728 -0.9085 -0.4180 -171.6999 -78.9945 30 131 3.6960 -0.8502 -0.5264 -111.3784 -68.9626 31 111 3.8192 -0.7791 -0.6269 -86.4779 -69.5885 32 104 3.9424 -0.6961 -0.7179 -72.3979 -74.6628 33 61 4.0656 -0.6026 -0.7980 -36.7607 -48.6791 34 91 4.1888 -0.5000 -0.8660 -45.5000 -78.8083 35 59 4.3120 -0.3898 -0.9209 -22.9974 -54.3334 36 69 4.4352 -0.2737 -0.9618 -18.8827 -66.3660 37 90 4.5584 -0.1534 -0.9882 -13.8052 -88.9349 38 81 4.6816 -0.0308 -0.9995 -2.4944 -80.9616 39 59 4.8048 0.0923 -0.9957 5.4438 -58.7483 40 63 4.9280 0.2139 -0.9768 13.4778 -61.5414 41 113 5.0512 0.3324 -0.9432 37.5561 -106.5765 42 67 5.1744 0.4457 -0.8952 29.8645 -59.9759 43 109 5.2976 0.5524 -0.8336 60.2078 -90.8627 44 51 5.4208 0.6506 -0.7594 33.1815 -38.7297 45 42 5.5440 0.7390 -0.6737 31.0384 -28.2952 46 65 5.6672 0.8162 -0.5778 53.0528 -37.5553 47 53 5.7904 0.8810 -0.4731 46.6936 -25.0740 48 50 5.9136 0.9325 -0.3612 46.6236 -18.0621 49 20 6.0368 0.9698 -0.2439 19.3959 -4.8783 50 22 6.1600 0.9924 -0.1229 21.8333 -2.7035 51 14 6.2832 1.0000 0.0000 14.0000 0.0000 TOTAL 6164 0.0000 0.0000 397.8217 1848.6629 12
  • 17. Table 2 shows that the calculations for Fourier series by using excel. From the table, we can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is 25.5 which is half of 51 (numbers of data). 1 51 a0   yk L k 1 6164  51  120.8627  51   nx     y k  cos      k 1   L   a1  L 397.8217  25.5  15.6009  51   nx     y k  sin       k 1   L   b1  L 1848.6629  25.5  72.4966 Then, we arrange the Fourier series as follow: 120.8627  x x  f ( x)   15.6009 cos  72.4966 sin   ... 2  25.5 25.5  13
  • 18. We can write the sum of sine and cosine term, with the same periodic which focus on the first harmonic by calculated the value of c0, c1 and α1. a0 c0  2 120.8627  2  60.4314 c1  a12  b12 ,  15.6009 2  72.4966 2  74.1562  a1   1  tan 1      b1   15.6009   tan 1    72.4966   0.2120 Then,  x  y  60.4314  74.1562 sin   L  0.2120    This equation is plotted by using Maple software to determine the peak value and analyze the trend of dengue cases. 14
  • 19. > > > Figure 4. Fourier series graph plotted for dengue cases in Gombak (2009) Figure 4 shows that Fourier series plotted with Maple software in first harmonic. The y- axis represents the number of dengue cases and the x-axis represents the number of weeks. From the graph, it shows that the maximum point or peak point in week 10 with 134 dengue cases. However, from week 32 to week 42, the graph shows that the minimum number of case which is zero. It happened because the different or gap between actual data for maximum cases and minimum cases is high. Early hypothesis from this graph is the highest cases happen in week 10 with 134 cases and the lowest cases happen between week 32 to week 42. 15
  • 20. Table 3. Fourier series calculations by using excel for dengue cases in Klang (2009) Week(x) Cases (y) (πx)/L cos (πx/L) sin (πx/L) [cos ((πx)/L )]*yk [sin ((πx)/L)] *yk 1 0 0.1232 0.9924 0.1229 0.0000 0.0000 2 116 0.2464 0.9698 0.2439 112.4964 28.2940 3 41 0.3696 0.9325 0.3612 38.2314 14.8109 4 64 0.4928 0.8810 0.4731 56.3848 30.2780 5 0 0.6160 0.8162 0.5778 0.0000 0.0000 6 22 0.7392 0.7390 0.6737 16.2582 14.8213 7 37 0.8624 0.6506 0.7594 24.0729 28.0980 8 49 0.9856 0.5524 0.8336 27.0659 40.8465 9 84 1.1088 0.4457 0.8952 37.4420 75.1937 10 78 1.2320 0.3324 0.9432 25.9237 73.5660 11 145 1.3552 0.2139 0.9768 31.0203 141.6430 12 189 1.4784 0.0923 0.9957 17.4387 188.1938 13 178 1.6016 -0.0308 0.9995 -5.4815 177.9156 14 210 1.7248 -0.1534 0.9882 -32.2122 207.5147 15 236 1.8480 -0.2737 0.9618 -64.5845 226.9909 16 334 1.9712 -0.3898 0.9209 -130.1885 307.5824 17 125 2.0944 -0.5000 0.8660 -62.5000 108.2532 18 178 2.2176 -0.6026 0.7980 -107.2690 142.0471 19 130 2.3408 -0.6961 0.7179 -90.4974 93.3285 20 109 2.4640 -0.7791 0.6269 -84.9198 68.3347 21 89 2.5872 -0.8502 0.5264 -75.6693 46.8525 22 60 2.7104 -0.9085 0.4180 -54.5079 25.0776 23 48 2.8336 -0.9529 0.3032 -45.7412 14.5513 24 20 2.9568 -0.9830 0.1837 -19.6595 3.6750 25 9 3.0800 -0.9981 0.0616 -8.9829 0.5540 26 9 3.2032 -0.9981 -0.0616 -8.9829 -0.5540 27 4 3.3264 -0.9830 -0.1837 -3.9319 -0.7350 28 6 3.4496 -0.9529 -0.3032 -5.7177 -1.8189 29 6 3.5728 -0.9085 -0.4180 -5.4508 -2.5078 30 0 3.6960 -0.8502 -0.5264 0.0000 0.0000 31 0 3.8192 -0.7791 -0.6269 0.0000 0.0000 32 0 3.9424 -0.6961 -0.7179 0.0000 0.0000 33 2 4.0656 -0.6026 -0.7980 -1.2053 -1.5960 34 0 4.1888 -0.5000 -0.8660 0.0000 0.0000 35 0 4.3120 -0.3898 -0.9209 0.0000 0.0000 36 0 4.4352 -0.2737 -0.9618 0.0000 0.0000 37 8 4.5584 -0.1534 -0.9882 -1.2271 -7.9053 38 0 4.6816 -0.0308 -0.9995 0.0000 0.0000 39 0 4.8048 0.0923 -0.9957 0.0000 0.0000 40 0 4.9280 0.2139 -0.9768 0.0000 0.0000 41 0 5.0512 0.3324 -0.9432 0.0000 0.0000 42 0 5.1744 0.4457 -0.8952 0.0000 0.0000 43 0 5.2976 0.5524 -0.8336 0.0000 0.0000 44 0 5.4208 0.6506 -0.7594 0.0000 0.0000 45 0 5.5440 0.7390 -0.6737 0.0000 0.0000 46 0 5.6672 0.8162 -0.5778 0.0000 0.0000 47 0 5.7904 0.8810 -0.4731 0.0000 0.0000 48 0 5.9136 0.9325 -0.3612 0.0000 0.0000 49 16 6.0368 0.9698 -0.2439 15.5168 -3.9026 50 8 6.1600 0.9924 -0.1229 7.9394 -0.9831 51 0 6.2832 1.0000 0.0000 0.0000 0.0000 TOTAL 2610 0.0000 0.0000 -398.9390 2038.4200 16
  • 21. Table 3 shows that the calculations for Fourier series by using excel. From the table, we can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is 25.5 which is half of 51 (numbers of data). 1 51 a0   yk L k 1 2610  51  51.1765  51   nx     y k  cos      k 1   L   a1  L  398.9390  25.5  15.6447  51   nx     y k  sin       k 1   L   b1  L 2038.4200  25.5  79.9380 Then, we arrange the Fourier series as follow: 51.1765  x x  f ( x)     15.6447 cos  79.9380 sin   ... 2  25.5 25.5  17
  • 22. We can write the sum of sine and cosine term, with the same periodic which focus on the first harmonic by calculated the value of c0, c1 and α1. a0 c0  2 51.1765  2  25.5882 c1  a12  b12 ,  (15.6447) 2  (79.9380) 2  81.4546  a1   1  tan 1      b1    15.6447   tan 1    79.9380   0.1933 Then,  x  y  25.5882  81.4546 sin  L  0.1933     This equation is plotted by using Maple software to determine the peak value and analyze the trend of dengue cases. 18
  • 23. > > > Figure 5. Fourier series graph plotted for dengue cases in Klang (2009) Figure 5 shows that Fourier series that plotted with Maple software in first harmonic. For y-axis represents the number of dengue cases and for x-axis represents the number of weeks. From the graph, it shows that the maximum point or peak point in week 15 with 120 dengue cases. However, from week 30 to week 50, the graph shows that the minimum number of case which is zero. It happened because the different or gap between actual data for maximum cases and minimum cases is high. Early hypothesis from this graph is the highest cases happen in week 15 with 120 cases and the lowest cases happen between weeks 30 to week 50. 19
  • 24. Table 4. Fourier series calculations for dengue cases in Shah Alam (2010) Week (x) Total (y) (πx)/L cos [(πx)/L] sin [(πx)/L] cos [(πx)/L] *Yk sin [(πx)/L] *Yk 1 56 0.2027 0.9795 0.2013 54.8537 11.2727 2 77 0.4054 0.9190 0.3944 70.7598 30.3654 3 85 0.6081 0.8208 0.5713 69.7649 48.5578 4 140 0.8107 0.6890 0.7248 96.4554 101.4710 5 168 1.0134 0.5290 0.8486 88.8660 142.5722 6 172 1.2161 0.3473 0.9378 59.7365 161.2934 7 168 1.4188 0.1514 0.9885 25.4399 166.0627 8 166 1.6215 -0.0506 0.9987 -8.4078 165.7869 9 162 1.8242 -0.2507 0.9681 -40.6057 156.8285 10 119 2.0268 -0.4404 0.8978 -52.4069 106.8387 11 109 2.2295 -0.6121 0.7908 -66.7196 86.1946 12 110 2.4322 -0.7588 0.6514 -83.4634 71.6510 13 61 2.6349 -0.8743 0.4853 -53.3351 29.6034 14 82 2.8376 -0.9541 0.2994 -78.2394 24.5478 15 74 3.0403 -0.9949 0.1012 -73.6203 7.4865 16 69 3.2429 -0.9949 -0.1012 -68.6460 -6.9806 17 44 3.4456 -0.9541 -0.2994 -41.9821 -13.1720 18 41 3.6483 -0.8743 -0.4853 -35.8482 -19.8974 19 14 3.8510 -0.7588 -0.6514 -10.6226 -9.1192 20 14 4.0537 -0.6121 -0.7908 -8.5695 -11.0709 21 10 4.2564 -0.4404 -0.8978 -4.4039 -8.9780 22 13 4.4590 -0.2507 -0.9681 -3.2585 -12.5850 23 5 4.6617 -0.0506 -0.9987 -0.2532 -4.9936 24 6 4.8644 0.1514 -0.9885 0.9086 -5.9308 25 22 5.0671 0.3473 -0.9378 7.6407 -20.6305 26 29 5.2698 0.5290 -0.8486 15.3400 -24.6107 27 34 5.4725 0.6890 -0.7248 23.4249 -24.6430 28 27 5.6751 0.8208 -0.5713 22.1606 -15.4242 29 21 5.8778 0.9190 -0.3944 19.2981 -8.2815 30 29 6.0805 0.9795 -0.2013 28.4064 -5.8377 31 23 6.2832 1.0000 0.0000 23.0000 0.0000 TOTAL 2150 0.0000 0.0000 -24.3271 1118.3775 20
  • 25. Table 4 shows that the calculations for Fourier series by using excel. From the table, we can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is 15.5 which is half of 31 (numbers of data). 1 31 a0   yk L k 1 2150  31  69.3548  31   nx     y k  cos      k 1   L   a1  L  24.3271  15.5  1.5695  31   nx     y k  sin       k 1   L   b1  L 1118.3775  15.5  72.1534 Then, we arrange the Fourier series as follow: 69.3548  x x  f ( x)     1.5695 cos  72.1534 sin   ... 2  15.5 15.5  21
  • 26. We can write the sum of sine and cosine term, with the same periodic which focus on the first harmonic by calculated the value of c0, c1 and α1. a0 c0  2 69.3548  2  34.6774 c1  a12  b12 ,  (1.5695) 2  (72.1534) 2  72.1705  a1   1  tan 1      b1    1.5695   tan 1    72.1534   0.0217 Then,  x  y  34.6774  72.1705 sin  L  0.0217     This equation is plotted by using Maple software to determine the peak value and analyze the trend of dengue cases. 22
  • 27. > > > Figure 6. Fourier series graph plotted for dengue cases in Shah Alam (2010) Figure 6 shows that Fourier series that plotted with Maple software in first harmonic. The y-axis represents the number of dengue cases and the x-axis represents the number of weeks. From the graph, it shows that the maximum point or peak point in week 9 with 120 dengue cases. However, from week 18 to week 28, the graph shows that the minimum number of case which is zero. It happened because the different or gap between actual data for maximum cases and minimum cases is high. Early hypothesis from this graph is the highest cases happen in week 9 with 120 cases and the lowest cases happen between week 18 to week 28. 23
  • 28. Table 5. Fourier series calculations by using excel for dengue cases in Gombak (2010) Week (x) Cases (y) (πx)/L cos [(πx)/L] sin [(πx)/L] [cos [(πx)/L]]*yk [sin [(πx)/L]] *yk 1 118 0.2027 0.9795 0.2013 115.5845 23.7532 2 126 0.4054 0.9190 0.3944 115.7887 49.6888 3 117 0.6081 0.8208 0.5713 96.0293 66.8384 4 184 0.8107 0.6890 0.7248 126.7699 133.3619 5 185 1.0134 0.5290 0.8486 97.8583 156.9992 6 184 1.2161 0.3473 0.9378 63.9042 172.5464 7 183 1.4188 0.1514 0.9885 27.7113 180.8897 8 174 1.6215 -0.0506 0.9987 -8.8130 173.7767 9 192 1.8242 -0.2507 0.9681 -48.1253 185.8708 10 180 2.0268 -0.4404 0.8978 -79.2709 161.6048 11 188 2.2295 -0.6121 0.7908 -115.0759 148.6658 12 166 2.4322 -0.7588 0.6514 -125.9538 108.1278 13 100 2.6349 -0.8743 0.4853 -87.4347 48.5302 14 125 2.8376 -0.9541 0.2994 -119.2674 37.4204 15 77 3.0403 -0.9949 0.1012 -76.6049 7.7900 16 92 3.2429 -0.9949 -0.1012 -91.5280 -9.3075 17 74 3.4456 -0.9541 -0.2994 -70.6063 -22.1529 18 67 3.6483 -0.8743 -0.4853 -58.5812 -32.5152 19 58 3.8510 -0.7588 -0.6514 -44.0080 -37.7796 20 52 4.0537 -0.6121 -0.7908 -31.8295 -41.1203 21 46 4.2564 -0.4404 -0.8978 -20.2581 -41.2990 22 46 4.4590 -0.2507 -0.9681 -11.5300 -44.5315 23 54 4.6617 -0.0506 -0.9987 -2.7351 -53.9307 24 55 4.8644 0.1514 -0.9885 8.3285 -54.3658 25 66 5.0671 0.3473 -0.9378 22.9221 -61.8916 26 67 5.2698 0.5290 -0.8486 35.4406 -56.8592 27 86 5.4725 0.6890 -0.7248 59.2512 -62.3322 28 109 5.6751 0.8208 -0.5713 89.4632 -62.2682 29 130 5.8778 0.9190 -0.3944 119.4645 -51.2663 30 138 6.0805 0.9795 -0.2013 135.1751 -27.7792 31 132 6.2832 1.0000 0.0000 132.0000 0.0000 TOTAL 3571 0.0000 0.0000 254.0694 996.4649 24
  • 29. Table 5 shows that the calculations for Fourier series by using excel. From the table, we can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is 15.5 which is half of 31 (numbers of data). 1 31 a0   yk L k 1 3571  31  115.1935  31   nx     y k  cos      k 1   L   a1  L 254.0694  15.5  16.3916  31   nx     y k  sin       k 1   L   b1  L 996.4649  15.5  64.2881 Then, we arrange the Fourier series as follow: 115.1935  x x  f ( x)   16.3981cos  64.2881sin   ... 2  15.5 15.5  25
  • 30. We can write the sum of sine and cosine term, with the same periodic which focus on the first harmonic by calculated the value of c0, c1 and α1. a0 c0  2 115.1935  2  57.5968 c1  a12  b12 ,  (16.3916) 2  (64.2881) 2  66.3448  a1   1  tan 1      b1   16.3916   tan 1    64.2881   0.2497 Then,  x  y  57.5968  66.3448 sin  L  0.2497     This equation is plotted by using Maple software to determine the peak value and analyze the trend of dengue cases. 26
  • 31. > > > Figure 7. Fourier series graph plotted for dengue cases in Gombak (2010) Figure 7 shows that Fourier series that plotted with Maple software in first harmonic. The y-axis represents the number of dengue cases and the x-axis represents the number of weeks. From the graph, it shows that the maximum point or peak point in week 7 with 120 dengue cases. However, from week 19 to week 24, the graph shows that the minimum number of case which is zero. It happened because the different or gap between actual data for maximum cases and minimum cases is high. Early hypothesis from this graph is the highest cases happen in week 7 with 120 cases and the lowest cases happen between week 19 to week 24. 27
  • 32. Table 6. Fourier series calculations by using excel for dengue cases in Klang (2010) Week(x) Total (y) (πx)/L cos (πx)/L sin (πx)/L [cos [(πx)/L]] *yk [sin [(πx)/L]] *yk 1 20 0.2027 0.9795 0.2013 19.5906 4.0260 2 14 0.4054 0.9190 0.3944 12.8654 5.5210 3 17 0.6081 0.8208 0.5713 13.9530 9.7116 4 40 0.8107 0.6890 0.7248 27.5587 28.9917 5 48 1.0134 0.5290 0.8486 25.3903 40.7349 6 47 1.2161 0.3473 0.9378 16.3233 44.0744 7 53 1.4188 0.1514 0.9885 8.0257 52.3888 8 59 1.6215 -0.0506 0.9987 -2.9883 58.9243 9 43 1.8242 -0.2507 0.9681 -10.7781 41.6273 10 53 2.0268 -0.4404 0.8978 -23.3409 47.5836 11 51 2.2295 -0.6121 0.7908 -31.2174 40.3296 12 47 2.4322 -0.7588 0.6514 -35.6616 30.6145 13 38 2.6349 -0.8743 0.4853 -33.2252 18.4415 14 41 2.8376 -0.9541 0.2994 -39.1197 12.2739 15 50 3.0403 -0.9949 0.1012 -49.7435 5.0584 16 53 3.2429 -0.9949 -0.1012 -52.7281 -5.3619 17 20 3.4456 -0.9541 -0.2994 -19.0828 -5.9873 18 25 3.6483 -0.8743 -0.4853 -21.8587 -12.1325 19 29 3.8510 -0.7588 -0.6514 -22.0040 -18.8898 20 24 4.0537 -0.6121 -0.7908 -14.6905 -18.9786 21 21 4.2564 -0.4404 -0.8978 -9.2483 -18.8539 22 12 4.4590 -0.2507 -0.9681 -3.0078 -11.6169 23 13 4.6617 -0.0506 -0.9987 -0.6584 -12.9833 24 14 4.8644 0.1514 -0.9885 2.1200 -13.8386 25 15 5.0671 0.3473 -0.9378 5.2096 -14.0663 26 19 5.2698 0.5290 -0.8486 10.0503 -16.1242 27 15 5.4725 0.6890 -0.7248 10.3345 -10.8719 28 16 5.6751 0.8208 -0.5713 13.1322 -9.1403 29 13 5.8778 0.9190 -0.3944 11.9465 -5.1266 30 31 6.0805 0.9795 -0.2013 30.3654 -6.2403 31 33 6.2832 1.0000 0.0000 33.0000 0.0000 TOTAL 974 0.0000 0.0000 -129.4878 260.0890 28
  • 33. Table 6 shows that the calculations for Fourier series by using excel. From the table, we can obtain coefficients of Fourier series which are a0, a1 and b1 where period time, L is 15.5 which is half of 31 (numbers of data). 1 31 a0   yk L k 1 974  31  31.4194  31   nx     y k  cos      k 1   L   a1  L  129.4878  15.5  8.3541  31   nx     y k  sin       k 1   L   b1  L 260.0890  15.5  16.7799 Then, we arrange the Fourier series as follow: 31.4194  x x  f ( x)     8.3541cos  16.7799 sin   ... 2  15.5 15.5  29
  • 34. We can write the sum of sine and cosine term, with the same periodic which focus on the first harmonic by calculated the value of c0, c1 and α1. a0 c0  2 31.4194  2  15.7097 c1  a12  b12 ,  (8.3541) 2  (16.7799) 2  18.7445  a1   1  tan 1      b1    8.3541   tan 1    16.7799   0.4619 Then,  x  y  15.7097  18.7445 sin  L  0.4619     This equation is plotted by using Maple software to determine the peak value and analyze the trend of dengue cases. 30
  • 35. > > > Figure 8. Fourier series graph plotted for dengue cases in Klang (2010) Figure 8 shows that Fourier series that plotted with Maple software in first harmonic. The y-axis represents the number of dengue cases and the x-axis represents the number of weeks. From the graph, it shows that the maximum point or peak point in week 10 with 35 dengue cases. However, from week 23 to week 28, the graph shows that the minimum number of case which is zero. It happened because the different or gap between actual data for maximum cases and minimum cases is high. Early hypothesis from this graph is the highest cases happen in week 10 with 35 cases and the lowest cases happen between week 23 to week 28. 31
  • 36. 4. RESULTS AND DISCUSSION From the findings, it can be noticed that the data of dengue cases in these three districts which are Shah Alam, Gombak and Klang is distributed fluctuation. It is difficult to determine and predict the dengue cases for the next year by following the trend line that is generated by Excel. Table 7. Fourier series equations on 1st harmonic for 2009 District Fourier Series Equation Shah Alam y= 80.4412 + 231.1922sin[(πx/25.5) + 0.3579] Gombak y= 60.4314 + 74.1562 sin[(πx/25.5) + 0.2120] Klang y= 25.5882 + 81.4546 sin[(πx/25.5) -0.1933] Table 8. Fourier series equations on 1st harmonic for 2010 District Fourier Series Equation Shah Alam y= 34.6774 + 72.1705sin [(πx/15.5) – 0.0217] Gombak y= 57.5968 + 66.344sin [(πx/15.5) +0.2497] Klang y= 15.7097 + 18.7445sin [(πx/15.5) – 0.4619] Table 9. Analysis from graph using maple software for 2009 District Peak Value Cases Week Shah Alam 310 10 Gombak 130 10 Klang 110 12 Table 10. Analysis from graph using maple software for 2010 District Peak Value Cases Week Shah Alam 120 9 Gombak 120 7 Klang 35 10 32
  • 37. The equation of Fourier series on first harmonic for dengue cases are shown in Table 7 and Table 8. For the year 2009, dengue cases seasonally peak between period week 10 to 14 (14 March 2009 until 11 April 2009) averagely recorded between 100 and 300 cases per week. It also shows that dengue cases dengue cases slowly decrease for chosen district at the end of year 2009. For the year 2010, dengue cases seasonally peak between period week 7 to week 10 (20 February 2010 until 13 March 2010) averagely recorded between 35 and 120 cases per week. It also shows that dengue cases dengue cases slowly decrease for chosen district started from week 18 to week 28 (8 May 2010 to 18 July). If we want to compare the result between year 2009 and 2010, we can see dengue cases seasonally peak at first quarter of year which averagely recorded in period week 7 to week 14 (February to April). Then, the dengue cases will reduce slowly in the third quarter of the year. 5. CONCLUSIONS AND RECOMMENDATIONS Dengue is one of the diseases with no specific treatment or immunizations. Thus, the preventive precautions from dengue such as fogging are important to reduce the cases. We can summarize that the peak dengue cases is peak between first quarter of the year which averagely recorded in period week 7 to week 14 (February to April). Shah Alam recorded the highest dengue cases in 2009 which 310 cases in week 10 compared to Klang which recorded 110. In year 2010, Shah Alam and Klang show drastic decrease the number of cases which 120 and 35 cases respectively. However, Gombak did not record the decrease cases in year 2010 compared to year 2009 which gives average of 120 cases. From the findings, it is recommended that the Ministry of Health Malaysia should focus more on first quarter of the year (February until April) every year to reduce dengue cases because this period recorded highest cases in 2009 and 2010. Further studies can be done for the previous year such as 2008 or 2007. So, the seasonal peak can be determined further. This model can be explored further by comparing the dengue cases recorded with climatic variability that is rainfalls, temperature and vapor pressure in those selected districts in Selangor. Comparison can also be done between states in Malaysia. 33
  • 38. REFERENCES Abas N., Daud Z.M., Yusof F. (2009). Fourier Series In A Temporal Rainfall Model. Proceeding of the 5th Asian Mathematical Conference, Malaysia. Ang, K.C. & Li, Zi. (1999). Modeling The Spread of Dengue in Singapore, Division of Mathematics, School of Sciences, Nanyang Technological University, Singapore. Angove, C. (2009). Some Discrete Real And Complex Fourier Transforms, A Discussion, With Examples. Favier, C., Degallier, N. & Dubois, M.A. (2005). Dengue Epidemic Modelling: Stakes and Pitfalls. Klingenberg, L. (2005). Frequency Domain Using Excel. San Francisco State University School of Engineering. Kvernadze, G., Hagstrom, T., and Shapiro, H. (2000). Detecting the Singularities of a Function of VP Class by its Integrated Fourier Series. Computers and Mathematics with Applications, 39, 25-43. McNeal, J. D. and Zeytuncu, Y. U. (2006). A note on rearrangement of Fourier series. J. Math. Anal. Appl. 323 (2006) 1348–1353. Nuraini, N., Soewono, E. & Sidarto, K.A. (2006). Mathematical Model of Dengue Disease Transmission with Severe DHF Compartment, Bulletin of the Malaysian Mathematical Sciences Society, 30, 143-157. Pongsumpun, P. & Tang, I.M. (2001). A Realistic Age Structure Transmission Model for Dengue Hemorrhagic Fever in Thailand, Department of Mathematics and Physics, Faculty of Sciences, Mahidol University. Tamrin, H., Riyanto, M.Z., Akhid Ardhian, A. (2007). Not Fatal Disease For SIR Model. Zill, D.G. & Cullen, M. R. (2009). Differential Equations With Boundary-Value Problems, 7th Edition, International Student Edition. 34