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EEEE 6490345 RF AND MICROWAVE ELECTRONICS
Transmission Line
FACULTY OF ENGINEERING AND COMPUTER TECHNOLOGY
BENG (HONS) IN ELECTRICALAND ELECTRONIC ENGINEERING
Ravandran Muttiah BEng (Hons) MSc MIET
Power
Example 1:
Consider the transmission line circuit shown in figure 1. Compute the
incident power, the reflected power and the power transmitted into the
infinite 75 Ω line. Show that power conservation is satisfied.
Figure 1: Transmission line circuit
1
50 Ω
𝑍1 = 75 Ω10 V 𝑍o = 50 Ω
λ 2
𝑃trans𝑃inc
𝑃ref
2
Solution:
𝑍in = 𝑍o
𝑍𝑙 + j𝑍o tan 𝛽𝑙
𝑍o + j𝑍𝑙 tan 𝛽𝑙
Since, 𝑙 =
λ
2
, tan 𝛽𝑙 = tan
2π
λ
λ
2
= tan π = 0
𝑍in = 𝑍o
𝑍𝑙 + 0
𝑍o + 0
𝑍𝑙 = 𝑍1 = 75 Ω
𝑅g = 50 Ω
𝑅L = 75 Ω𝑉g = 10 V
Source impedance
Terminal
impedance
Characteristics
impedance
𝑍o = 50 Ω
𝐼g
+ -
+
-
Figure 2
3
Power delivered by source =
1
2
𝑉g 𝐼g cos 𝜃
𝑍in =
1
2
10
10
50 + 75
=
1
2
100
125
= 0.4W
Power dissipated in 50 Ω,
𝑃r =
1
2
𝐼g
2
𝑅g =
1
2
10
50 + 75
2
50 = 0.16W
Power transmitted down the line or Power delivered to load 𝑃L,
𝑃L =
1
2
𝐼g
2
𝑅L
=
1
2
10
50 + 75
2
75
= 0.24 W
4
Incident power is also the input power.
𝑃inc =
1
2
𝐼g
2
𝑍o
=
1
2
10
50 + 50
2
50
= 0.25 W
50 Ω
50 Ω𝑉g = 10 V 𝑍o = 50 Ω
𝐼g
+ -
+
-
Figure 3
𝑃inc
5
𝑅g = 50 Ω
𝑅L = 75 Ω𝑉g
S11 or Гin
𝐼g
+ -
+
-
Figure 4
Input reflection coefficient, Гin =
75 − 50
75 + 50
=
25
125
= 0.4
Reflected power, 𝑃r = 𝑃inc Гin = 0.25 0.4 = 0.1 W
Transmitted power = Incident power – Reflected power = 0.25 − 0.1 W
= 0.24 W
Power from source, 𝑃g = Dissipated power + Transmitted power
= 0.16 + 0.24 W = 0.4 W

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Lecture Notes: EEEE6490345 RF and Microwave Electronics - Transmission Line

  • 1. EEEE 6490345 RF AND MICROWAVE ELECTRONICS Transmission Line FACULTY OF ENGINEERING AND COMPUTER TECHNOLOGY BENG (HONS) IN ELECTRICALAND ELECTRONIC ENGINEERING Ravandran Muttiah BEng (Hons) MSc MIET
  • 2. Power Example 1: Consider the transmission line circuit shown in figure 1. Compute the incident power, the reflected power and the power transmitted into the infinite 75 Ω line. Show that power conservation is satisfied. Figure 1: Transmission line circuit 1 50 Ω 𝑍1 = 75 Ω10 V 𝑍o = 50 Ω λ 2 𝑃trans𝑃inc 𝑃ref
  • 3. 2 Solution: 𝑍in = 𝑍o 𝑍𝑙 + j𝑍o tan 𝛽𝑙 𝑍o + j𝑍𝑙 tan 𝛽𝑙 Since, 𝑙 = λ 2 , tan 𝛽𝑙 = tan 2π λ λ 2 = tan π = 0 𝑍in = 𝑍o 𝑍𝑙 + 0 𝑍o + 0 𝑍𝑙 = 𝑍1 = 75 Ω 𝑅g = 50 Ω 𝑅L = 75 Ω𝑉g = 10 V Source impedance Terminal impedance Characteristics impedance 𝑍o = 50 Ω 𝐼g + - + - Figure 2
  • 4. 3 Power delivered by source = 1 2 𝑉g 𝐼g cos 𝜃 𝑍in = 1 2 10 10 50 + 75 = 1 2 100 125 = 0.4W Power dissipated in 50 Ω, 𝑃r = 1 2 𝐼g 2 𝑅g = 1 2 10 50 + 75 2 50 = 0.16W Power transmitted down the line or Power delivered to load 𝑃L, 𝑃L = 1 2 𝐼g 2 𝑅L = 1 2 10 50 + 75 2 75 = 0.24 W
  • 5. 4 Incident power is also the input power. 𝑃inc = 1 2 𝐼g 2 𝑍o = 1 2 10 50 + 50 2 50 = 0.25 W 50 Ω 50 Ω𝑉g = 10 V 𝑍o = 50 Ω 𝐼g + - + - Figure 3 𝑃inc
  • 6. 5 𝑅g = 50 Ω 𝑅L = 75 Ω𝑉g S11 or Гin 𝐼g + - + - Figure 4 Input reflection coefficient, Гin = 75 − 50 75 + 50 = 25 125 = 0.4 Reflected power, 𝑃r = 𝑃inc Гin = 0.25 0.4 = 0.1 W Transmitted power = Incident power – Reflected power = 0.25 − 0.1 W = 0.24 W Power from source, 𝑃g = Dissipated power + Transmitted power = 0.16 + 0.24 W = 0.4 W