SlideShare una empresa de Scribd logo
1 de 90
Descargar para leer sin conexión
Section 3.4
Exponential Growth and Decay
V63.0121.021, Calculus I
New York University
October 28, 2010
Announcements
Quiz 3 next week in recitation on 2.6, 2.8, 3.1, 3.2
. . . . . .
. . . . . .
Announcements
Quiz 3 next week in
recitation on 2.6, 2.8, 3.1,
3.2
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 2 / 40
. . . . . .
Objectives
Solve the ordinary
differential equation
y′
(t) = ky(t), y(0) = y0
Solve problems involving
exponential growth and
decay
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 3 / 40
. . . . . .
Outline
Recall
The differential equation y′
= ky
Modeling simple population growth
Modeling radioactive decay
Carbon-14 Dating
Newton’s Law of Cooling
Continuously Compounded Interest
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 4 / 40
. . . . . .
Derivatives of exponential and logarithmic functions
y y′
ex
ex
ax
(ln a) · ax
ln x
1
x
loga x
1
ln a
·
1
x
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 5 / 40
. . . . . .
Outline
Recall
The differential equation y′
= ky
Modeling simple population growth
Modeling radioactive decay
Carbon-14 Dating
Newton’s Law of Cooling
Continuously Compounded Interest
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 6 / 40
. . . . . .
What is a differential equation?
Definition
A differential equation is an equation for an unknown function which
includes the function and its derivatives.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 7 / 40
. . . . . .
What is a differential equation?
Definition
A differential equation is an equation for an unknown function which
includes the function and its derivatives.
Example
Newton’s Second Law F = ma is a differential equation, where
a(t) = x′′
(t).
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 7 / 40
. . . . . .
What is a differential equation?
Definition
A differential equation is an equation for an unknown function which
includes the function and its derivatives.
Example
Newton’s Second Law F = ma is a differential equation, where
a(t) = x′′
(t).
In a spring, F(x) = −kx, where x is displacement from equilibrium
and k is a constant. So
−kx(t) = mx′′
(t) =⇒ x′′
(t) +
k
m
x(t) = 0.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 7 / 40
. . . . . .
What is a differential equation?
Definition
A differential equation is an equation for an unknown function which
includes the function and its derivatives.
Example
Newton’s Second Law F = ma is a differential equation, where
a(t) = x′′
(t).
In a spring, F(x) = −kx, where x is displacement from equilibrium
and k is a constant. So
−kx(t) = mx′′
(t) =⇒ x′′
(t) +
k
m
x(t) = 0.
The most general solution is x(t) = A sin ωt + B cos ωt, where
ω =
√
k/m.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 7 / 40
. . . . . .
Showing a function is a solution
Example (Continued)
Show that x(t) = A sin ωt + B cos ωt satisfies the differential equation
x′′
+
k
m
x = 0, where ω =
√
k/m.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 8 / 40
. . . . . .
Showing a function is a solution
Example (Continued)
Show that x(t) = A sin ωt + B cos ωt satisfies the differential equation
x′′
+
k
m
x = 0, where ω =
√
k/m.
Solution
We have
x(t) = A sin ωt + B cos ωt
x′
(t) = Aω cos ωt − Bω sin ωt
x′′
(t) = −Aω2
sin ωt − Bω2
cos ωt
Since ω2
= k/m, the last line plus k/m times the first line result in zero.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 8 / 40
. . . . . .
The Equation y′
= 2
Example
Find a solution to y′
(t) = 2.
Find the most general solution to y′
(t) = 2.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 9 / 40
. . . . . .
The Equation y′
= 2
Example
Find a solution to y′
(t) = 2.
Find the most general solution to y′
(t) = 2.
Solution
A solution is y(t) = 2t.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 9 / 40
. . . . . .
The Equation y′
= 2
Example
Find a solution to y′
(t) = 2.
Find the most general solution to y′
(t) = 2.
Solution
A solution is y(t) = 2t.
The general solution is y = 2t + C.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 9 / 40
. . . . . .
The Equation y′
= 2
Example
Find a solution to y′
(t) = 2.
Find the most general solution to y′
(t) = 2.
Solution
A solution is y(t) = 2t.
The general solution is y = 2t + C.
Remark
If a function has a constant rate of growth, it’s linear.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 9 / 40
. . . . . .
The Equation y′
= 2t
Example
Find a solution to y′
(t) = 2t.
Find the most general solution to y′
(t) = 2t.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 10 / 40
. . . . . .
The Equation y′
= 2t
Example
Find a solution to y′
(t) = 2t.
Find the most general solution to y′
(t) = 2t.
Solution
A solution is y(t) = t2
.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 10 / 40
. . . . . .
The Equation y′
= 2t
Example
Find a solution to y′
(t) = 2t.
Find the most general solution to y′
(t) = 2t.
Solution
A solution is y(t) = t2
.
The general solution is y = t2
+ C.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 10 / 40
. . . . . .
The Equation y′
= y
Example
Find a solution to y′
(t) = y(t).
Find the most general solution to y′
(t) = y(t).
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 11 / 40
. . . . . .
The Equation y′
= y
Example
Find a solution to y′
(t) = y(t).
Find the most general solution to y′
(t) = y(t).
Solution
A solution is y(t) = et
.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 11 / 40
. . . . . .
The Equation y′
= y
Example
Find a solution to y′
(t) = y(t).
Find the most general solution to y′
(t) = y(t).
Solution
A solution is y(t) = et
.
The general solution is y = Cet
, not y = et
+ C.
(check this)
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 11 / 40
. . . . . .
Kick it up a notch: y′
= 2y
Example
Find a solution to y′
= 2y.
Find the general solution to y′
= 2y.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 12 / 40
. . . . . .
Kick it up a notch: y′
= 2y
Example
Find a solution to y′
= 2y.
Find the general solution to y′
= 2y.
Solution
y = e2t
y = Ce2t
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 12 / 40
. . . . . .
In general: y′
= ky
Example
Find a solution to y′
= ky.
Find the general solution to y′
= ky.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 13 / 40
. . . . . .
In general: y′
= ky
Example
Find a solution to y′
= ky.
Find the general solution to y′
= ky.
Solution
y = ekt
y = Cekt
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 13 / 40
. . . . . .
In general: y′
= ky
Example
Find a solution to y′
= ky.
Find the general solution to y′
= ky.
Solution
y = ekt
y = Cekt
Remark
What is C? Plug in t = 0:
y(0) = Cek·0
= C · 1 = C,
so y(0) = y0, the initial value of y.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 13 / 40
. . . . . .
Constant Relative Growth =⇒ Exponential Growth
Theorem
A function with constant relative growth rate k is an exponential
function with parameter k. Explicitly, the solution to the equation
y′
(t) = ky(t) y(0) = y0
is
y(t) = y0ekt
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 14 / 40
. . . . . .
Exponential Growth is everywhere
Lots of situations have growth rates proportional to the current
value
This is the same as saying the relative growth rate is constant.
Examples: Natural population growth, compounded interest,
social networks
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 15 / 40
. . . . . .
Outline
Recall
The differential equation y′
= ky
Modeling simple population growth
Modeling radioactive decay
Carbon-14 Dating
Newton’s Law of Cooling
Continuously Compounded Interest
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 16 / 40
. . . . . .
Bacteria
Since you need bacteria to
make bacteria, the amount
of new bacteria at any
moment is proportional to
the total amount of
bacteria.
This means bacteria
populations grow
exponentially.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 17 / 40
. . . . . .
Bacteria Example
Example
A colony of bacteria is grown under ideal conditions in a laboratory. At
the end of 3 hours there are 10,000 bacteria. At the end of 5 hours
there are 40,000. How many bacteria were present initially?
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 18 / 40
. . . . . .
Bacteria Example
Example
A colony of bacteria is grown under ideal conditions in a laboratory. At
the end of 3 hours there are 10,000 bacteria. At the end of 5 hours
there are 40,000. How many bacteria were present initially?
Solution
Since y′
= ky for bacteria, we have y = y0ekt
. We have
10, 000 = y0ek·3
40, 000 = y0ek·5
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 18 / 40
. . . . . .
Bacteria Example
Example
A colony of bacteria is grown under ideal conditions in a laboratory. At
the end of 3 hours there are 10,000 bacteria. At the end of 5 hours
there are 40,000. How many bacteria were present initially?
Solution
Since y′
= ky for bacteria, we have y = y0ekt
. We have
10, 000 = y0ek·3
40, 000 = y0ek·5
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 18 / 40
. . . . . .
Bacteria Example
Example
A colony of bacteria is grown under ideal conditions in a laboratory. At
the end of 3 hours there are 10,000 bacteria. At the end of 5 hours
there are 40,000. How many bacteria were present initially?
Solution
Since y′
= ky for bacteria, we have y = y0ekt
. We have
10, 000 = y0ek·3
40, 000 = y0ek·5
Dividing the first into the second gives
4 = e2k
=⇒ 2k = ln 4 =⇒ k = ln 2. Now we have
10, 000 = y0eln 2·3
= y0 · 8
So y0 =
10, 000
8
= 1250.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 18 / 40
. . . . . .
Could you do that again please?
We have
10, 000 = y0ek·3
40, 000 = y0ek·5
Dividing the first into the second gives
40, 000
10, 000
=
y0e5k
y0e3k
=⇒ 4 = e2k
=⇒ ln 4 = ln(e2k
) = 2k
=⇒ k =
ln 4
2
=
ln 22
2
=
2 ln 2
2
= ln 2
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 19 / 40
. . . . . .
Outline
Recall
The differential equation y′
= ky
Modeling simple population growth
Modeling radioactive decay
Carbon-14 Dating
Newton’s Law of Cooling
Continuously Compounded Interest
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 20 / 40
. . . . . .
Modeling radioactive decay
Radioactive decay occurs because many large atoms spontaneously
give off particles.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 21 / 40
. . . . . .
Modeling radioactive decay
Radioactive decay occurs because many large atoms spontaneously
give off particles.
This means that in a sample of
a bunch of atoms, we can
assume a certain percentage of
them will “go off” at any point.
(For instance, if all atom of a
certain radioactive element
have a 20% chance of decaying
at any point, then we can
expect in a sample of 100 that
20 of them will be decaying.)
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 21 / 40
. . . . . .
Radioactive decay as a differential equation
The relative rate of decay is constant:
y′
y
= k
where k is negative.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 22 / 40
. . . . . .
Radioactive decay as a differential equation
The relative rate of decay is constant:
y′
y
= k
where k is negative. So
y′
= ky =⇒ y = y0ekt
again!
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 22 / 40
. . . . . .
Radioactive decay as a differential equation
The relative rate of decay is constant:
y′
y
= k
where k is negative. So
y′
= ky =⇒ y = y0ekt
again!
It’s customary to express the relative rate of decay in the units of
half-life: the amount of time it takes a pure sample to decay to one
which is only half pure.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 22 / 40
. . . . . .
Computing the amount remaining of a decaying
sample
Example
The half-life of polonium-210 is about 138 days. How much of a 100 g
sample remains after t years?
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 23 / 40
. . . . . .
Computing the amount remaining of a decaying
sample
Example
The half-life of polonium-210 is about 138 days. How much of a 100 g
sample remains after t years?
Solution
We have y = y0ekt
, where y0 = y(0) = 100 grams. Then
50 = 100ek·138/365
=⇒ k = −
365 · ln 2
138
.
Therefore
y(t) = 100e−365·ln 2
138
t
= 100 · 2−365t/138
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 23 / 40
. . . . . .
Computing the amount remaining of a decaying
sample
Example
The half-life of polonium-210 is about 138 days. How much of a 100 g
sample remains after t years?
Solution
We have y = y0ekt
, where y0 = y(0) = 100 grams. Then
50 = 100ek·138/365
=⇒ k = −
365 · ln 2
138
.
Therefore
y(t) = 100e−365·ln 2
138
t
= 100 · 2−365t/138
Notice y(t) = y0 · 2−t/t1/2 , where t1/2 is the half-life.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 23 / 40
. . . . . .
Carbon-14 Dating
The ratio of carbon-14 to
carbon-12 in an organism
decays exponentially:
p(t) = p0e−kt
.
The half-life of carbon-14 is
about 5700 years. So the
equation for p(t) is
p(t) = p0e− ln2
5700
t
Another way to write this would
be
p(t) = p02−t/5700
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 24 / 40
. . . . . .
Computing age with Carbon-14 content
Example
Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is
10% of that in a living organism. How old is the fossil?
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
. . . . . .
Computing age with Carbon-14 content
Example
Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is
10% of that in a living organism. How old is the fossil?
Solution
We are looking for the value of t for which
p(t)
p0
= 0.1
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
. . . . . .
Computing age with Carbon-14 content
Example
Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is
10% of that in a living organism. How old is the fossil?
Solution
We are looking for the value of t for which
p(t)
p0
= 0.1 From the
equation we have
2−t/5700
= 0.1
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
. . . . . .
Computing age with Carbon-14 content
Example
Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is
10% of that in a living organism. How old is the fossil?
Solution
We are looking for the value of t for which
p(t)
p0
= 0.1 From the
equation we have
2−t/5700
= 0.1 =⇒ −
t
5700
ln 2 = ln 0.1
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
. . . . . .
Computing age with Carbon-14 content
Example
Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is
10% of that in a living organism. How old is the fossil?
Solution
We are looking for the value of t for which
p(t)
p0
= 0.1 From the
equation we have
2−t/5700
= 0.1 =⇒ −
t
5700
ln 2 = ln 0.1 =⇒ t =
ln 0.1
ln 2
· 5700
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
. . . . . .
Computing age with Carbon-14 content
Example
Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is
10% of that in a living organism. How old is the fossil?
Solution
We are looking for the value of t for which
p(t)
p0
= 0.1 From the
equation we have
2−t/5700
= 0.1 =⇒ −
t
5700
ln 2 = ln 0.1 =⇒ t =
ln 0.1
ln 2
· 5700 ≈ 18, 940
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
. . . . . .
Computing age with Carbon-14 content
Example
Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is
10% of that in a living organism. How old is the fossil?
Solution
We are looking for the value of t for which
p(t)
p0
= 0.1 From the
equation we have
2−t/5700
= 0.1 =⇒ −
t
5700
ln 2 = ln 0.1 =⇒ t =
ln 0.1
ln 2
· 5700 ≈ 18, 940
So the fossil is almost 19,000 years old.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
. . . . . .
Outline
Recall
The differential equation y′
= ky
Modeling simple population growth
Modeling radioactive decay
Carbon-14 Dating
Newton’s Law of Cooling
Continuously Compounded Interest
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 26 / 40
. . . . . .
Newton's Law of Cooling
Newton’s Law of Cooling
states that the rate of
cooling of an object is
proportional to the
temperature difference
between the object and its
surroundings.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 27 / 40
. . . . . .
Newton's Law of Cooling
Newton’s Law of Cooling
states that the rate of
cooling of an object is
proportional to the
temperature difference
between the object and its
surroundings.
This gives us a differential
equation of the form
dT
dt
= k(T − Ts)
(where k < 0 again).
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 27 / 40
. . . . . .
General Solution to NLC problems
To solve this, change the variable y(t) = T(t) − Ts. Then y′
= T′
and
k(T − Ts) = ky. The equation now looks like
dT
dt
= k(T − Ts) ⇐⇒
dy
dt
= ky
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
. . . . . .
General Solution to NLC problems
To solve this, change the variable y(t) = T(t) − Ts. Then y′
= T′
and
k(T − Ts) = ky. The equation now looks like
dT
dt
= k(T − Ts) ⇐⇒
dy
dt
= ky
Now we can solve!
y′
= ky
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
. . . . . .
General Solution to NLC problems
To solve this, change the variable y(t) = T(t) − Ts. Then y′
= T′
and
k(T − Ts) = ky. The equation now looks like
dT
dt
= k(T − Ts) ⇐⇒
dy
dt
= ky
Now we can solve!
y′
= ky =⇒ y = Cekt
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
. . . . . .
General Solution to NLC problems
To solve this, change the variable y(t) = T(t) − Ts. Then y′
= T′
and
k(T − Ts) = ky. The equation now looks like
dT
dt
= k(T − Ts) ⇐⇒
dy
dt
= ky
Now we can solve!
y′
= ky =⇒ y = Cekt
=⇒ T − Ts = Cekt
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
. . . . . .
General Solution to NLC problems
To solve this, change the variable y(t) = T(t) − Ts. Then y′
= T′
and
k(T − Ts) = ky. The equation now looks like
dT
dt
= k(T − Ts) ⇐⇒
dy
dt
= ky
Now we can solve!
y′
= ky =⇒ y = Cekt
=⇒ T − Ts = Cekt
=⇒ T = Cekt
+ Ts
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
. . . . . .
General Solution to NLC problems
To solve this, change the variable y(t) = T(t) − Ts. Then y′
= T′
and
k(T − Ts) = ky. The equation now looks like
dT
dt
= k(T − Ts) ⇐⇒
dy
dt
= ky
Now we can solve!
y′
= ky =⇒ y = Cekt
=⇒ T − Ts = Cekt
=⇒ T = Cekt
+ Ts
Plugging in t = 0, we see C = y0 = T0 − Ts. So
Theorem
The solution to the equation T′
(t) = k(T(t) − Ts), T(0) = T0 is
T(t) = (T0 − Ts)ekt
+ Ts
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
. . . . . .
Computing cooling time with NLC
Example
A hard-boiled egg at 98 ◦
C is put in a sink of 18 ◦
C water. After 5
minutes, the egg’s temperature is 38 ◦
C. Assuming the water has not
warmed appreciably, how much longer will it take the egg to reach
20 ◦
C?
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 29 / 40
. . . . . .
Computing cooling time with NLC
Example
A hard-boiled egg at 98 ◦
C is put in a sink of 18 ◦
C water. After 5
minutes, the egg’s temperature is 38 ◦
C. Assuming the water has not
warmed appreciably, how much longer will it take the egg to reach
20 ◦
C?
Solution
We know that the temperature function takes the form
T(t) = (T0 − Ts)ekt
+ Ts = 80ekt
+ 18
To find k, plug in t = 5:
38 = T(5) = 80e5k
+ 18
and solve for k.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 29 / 40
. . . . . .
Finding k
Solution (Continued)
38 = T(5) = 80e5k
+ 18
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
. . . . . .
Finding k
Solution (Continued)
38 = T(5) = 80e5k
+ 18
20 = 80e5k
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
. . . . . .
Finding k
Solution (Continued)
38 = T(5) = 80e5k
+ 18
20 = 80e5k
1
4
= e5k
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
. . . . . .
Finding k
Solution (Continued)
38 = T(5) = 80e5k
+ 18
20 = 80e5k
1
4
= e5k
ln
(
1
4
)
= 5k
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
. . . . . .
Finding k
Solution (Continued)
38 = T(5) = 80e5k
+ 18
20 = 80e5k
1
4
= e5k
ln
(
1
4
)
= 5k
=⇒ k = −
1
5
ln 4.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
. . . . . .
Finding k
Solution (Continued)
38 = T(5) = 80e5k
+ 18
20 = 80e5k
1
4
= e5k
ln
(
1
4
)
= 5k
=⇒ k = −
1
5
ln 4.
Now we need to solve for t:
20 = T(t) = 80e− t
5
ln 4
+ 18
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
. . . . . .
Finding t
Solution (Continued)
20 = 80e− t
5
ln 4
+ 18
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
. . . . . .
Finding t
Solution (Continued)
20 = 80e− t
5
ln 4
+ 18
2 = 80e− t
5
ln 4
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
. . . . . .
Finding t
Solution (Continued)
20 = 80e− t
5
ln 4
+ 18
2 = 80e− t
5
ln 4
1
40
= e− t
5
ln 4
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
. . . . . .
Finding t
Solution (Continued)
20 = 80e− t
5
ln 4
+ 18
2 = 80e− t
5
ln 4
1
40
= e− t
5
ln 4
− ln 40 = −
t
5
ln 4
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
. . . . . .
Finding t
Solution (Continued)
20 = 80e− t
5
ln 4
+ 18
2 = 80e− t
5
ln 4
1
40
= e− t
5
ln 4
− ln 40 = −
t
5
ln 4
=⇒ t =
ln 40
1
5 ln 4
=
5 ln 40
ln 4
≈ 13 min
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
. . . . . .
Computing time of death with NLC
Example
A murder victim is discovered at
midnight and the temperature of
the body is recorded as 31 ◦
C.
One hour later, the temperature
of the body is 29 ◦
C. Assume
that the surrounding air
temperature remains constant
at 21 ◦
C. Calculate the victim’s
time of death. (The “normal”
temperature of a living human
being is approximately 37 ◦
C.)
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 32 / 40
. . . . . .
Solution
Let time 0 be midnight. We know T0 = 31, Ts = 21, and
T(1) = 29. We want to know the t for which T(t) = 37.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 33 / 40
. . . . . .
Solution
Let time 0 be midnight. We know T0 = 31, Ts = 21, and
T(1) = 29. We want to know the t for which T(t) = 37.
To find k:
29 = 10ek·1
+ 21 =⇒ k = ln 0.8
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 33 / 40
. . . . . .
Solution
Let time 0 be midnight. We know T0 = 31, Ts = 21, and
T(1) = 29. We want to know the t for which T(t) = 37.
To find k:
29 = 10ek·1
+ 21 =⇒ k = ln 0.8
To find t:
37 = 10et·ln(0.8)
+ 21
1.6 = et·ln(0.8)
t =
ln(1.6)
ln(0.8)
≈ −2.10 hr
So the time of death was just before 10:00pm.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 33 / 40
. . . . . .
Outline
Recall
The differential equation y′
= ky
Modeling simple population growth
Modeling radioactive decay
Carbon-14 Dating
Newton’s Law of Cooling
Continuously Compounded Interest
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 34 / 40
. . . . . .
Interest
If an account has an compound interest rate of r per year
compounded n times, then an initial deposit of A0 dollars becomes
A0
(
1 +
r
n
)nt
after t years.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 35 / 40
. . . . . .
Interest
If an account has an compound interest rate of r per year
compounded n times, then an initial deposit of A0 dollars becomes
A0
(
1 +
r
n
)nt
after t years.
For different amounts of compounding, this will change. As
n → ∞, we get continously compounded interest
A(t) = lim
n→∞
A0
(
1 +
r
n
)nt
= A0ert
.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 35 / 40
. . . . . .
Interest
If an account has an compound interest rate of r per year
compounded n times, then an initial deposit of A0 dollars becomes
A0
(
1 +
r
n
)nt
after t years.
For different amounts of compounding, this will change. As
n → ∞, we get continously compounded interest
A(t) = lim
n→∞
A0
(
1 +
r
n
)nt
= A0ert
.
Thus dollars are like bacteria.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 35 / 40
. . . . . .
Continuous vs. Discrete Compounding of interest
Example
Consider two bank accounts: one with 10% annual interested
compounded quarterly and one with annual interest rate r compunded
continuously. If they produce the same balance after every year, what
is r?
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 36 / 40
. . . . . .
Continuous vs. Discrete Compounding of interest
Example
Consider two bank accounts: one with 10% annual interested
compounded quarterly and one with annual interest rate r compunded
continuously. If they produce the same balance after every year, what
is r?
Solution
The balance for the 10% compounded quarterly account after t years is
A1(t) = A0(1.025)4t
= P((1.025)4
)t
The balance for the interest rate r compounded continuously account
after t years is
A2(t) = A0ert
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 36 / 40
. . . . . .
Solving
Solution (Continued)
A1(t) = A0((1.025)4
)t
A2(t) = A0(er
)t
For those to be the same, er
= (1.025)4
, so
r = ln((1.025)4
) = 4 ln 1.025 ≈ 0.0988
So 10% annual interest compounded quarterly is basically equivalent
to 9.88% compounded continuously.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 37 / 40
. . . . . .
Computing doubling time with exponential growth
Example
How long does it take an initial deposit of $100, compounded
continuously, to double?
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 38 / 40
. . . . . .
Computing doubling time with exponential growth
Example
How long does it take an initial deposit of $100, compounded
continuously, to double?
Solution
We need t such that A(t) = 200. In other words
200 = 100ert
=⇒ 2 = ert
=⇒ ln 2 = rt =⇒ t =
ln 2
r
.
For instance, if r = 6% = 0.06, we have
t =
ln 2
0.06
≈
0.69
0.06
=
69
6
= 11.5 years.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 38 / 40
. . . . . .
I-banking interview tip of the day
The fraction
ln 2
r
can also
be approximated as either
70 or 72 divided by the
percentage rate (as a
number between 0 and
100, not a fraction between
0 and 1.)
This is sometimes called
the rule of 70 or rule of 72.
72 has lots of factors so it’s
used more often.
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 39 / 40
. . . . . .
Summary
When something grows or decays at a constant relative rate, the
growth or decay is exponential.
Equations with unknowns in an exponent can be solved with
logarithms.
Your friend list is like culture of bacteria (no offense).
V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 40 / 40

Más contenido relacionado

La actualidad más candente

Ordinary differential equations
Ordinary differential equationsOrdinary differential equations
Ordinary differential equationsAhmed Haider
 
Laplace Transformation & Its Application
Laplace Transformation & Its ApplicationLaplace Transformation & Its Application
Laplace Transformation & Its ApplicationChandra Kundu
 
Differential equations
Differential equationsDifferential equations
Differential equationsSeyid Kadher
 
ORDINARY DIFFERENTIAL EQUATION
ORDINARY DIFFERENTIAL EQUATION ORDINARY DIFFERENTIAL EQUATION
ORDINARY DIFFERENTIAL EQUATION LANKESH S S
 
Diagonalization of Matrices
Diagonalization of MatricesDiagonalization of Matrices
Diagonalization of MatricesAmenahGondal1
 
Differential equations
Differential equationsDifferential equations
Differential equationsUzair Saiyed
 
Linear differential equation with constant coefficient
Linear differential equation with constant coefficientLinear differential equation with constant coefficient
Linear differential equation with constant coefficientSanjay Singh
 
Homogeneous Linear Differential Equations
 Homogeneous Linear Differential Equations Homogeneous Linear Differential Equations
Homogeneous Linear Differential EquationsAMINULISLAM439
 
Ode powerpoint presentation1
Ode powerpoint presentation1Ode powerpoint presentation1
Ode powerpoint presentation1Pokkarn Narkhede
 
LINEAR DIFFERENTIAL EQUATION AND BERNOULLIS EQUATIONS
LINEAR DIFFERENTIAL EQUATION AND BERNOULLIS EQUATIONSLINEAR DIFFERENTIAL EQUATION AND BERNOULLIS EQUATIONS
LINEAR DIFFERENTIAL EQUATION AND BERNOULLIS EQUATIONSParthivpal17
 
Divergence,curl,gradient
Divergence,curl,gradientDivergence,curl,gradient
Divergence,curl,gradientKunj Patel
 
euler's theorem
euler's theoremeuler's theorem
euler's theoremmihir jain
 
introduction to differential equations
introduction to differential equationsintroduction to differential equations
introduction to differential equationsEmdadul Haque Milon
 
Complex function
Complex functionComplex function
Complex functionShrey Patel
 
PPT of Improper Integrals IMPROPER INTEGRAL
PPT of Improper Integrals IMPROPER INTEGRALPPT of Improper Integrals IMPROPER INTEGRAL
PPT of Improper Integrals IMPROPER INTEGRALHanuwantSingh Dewal
 

La actualidad más candente (20)

Ordinary differential equations
Ordinary differential equationsOrdinary differential equations
Ordinary differential equations
 
Laplace Transformation & Its Application
Laplace Transformation & Its ApplicationLaplace Transformation & Its Application
Laplace Transformation & Its Application
 
Differential equations
Differential equationsDifferential equations
Differential equations
 
ORDINARY DIFFERENTIAL EQUATION
ORDINARY DIFFERENTIAL EQUATION ORDINARY DIFFERENTIAL EQUATION
ORDINARY DIFFERENTIAL EQUATION
 
Diagonalization of Matrices
Diagonalization of MatricesDiagonalization of Matrices
Diagonalization of Matrices
 
Differential equations
Differential equationsDifferential equations
Differential equations
 
Differential equations
Differential equationsDifferential equations
Differential equations
 
Linear differential equation with constant coefficient
Linear differential equation with constant coefficientLinear differential equation with constant coefficient
Linear differential equation with constant coefficient
 
Homogeneous Linear Differential Equations
 Homogeneous Linear Differential Equations Homogeneous Linear Differential Equations
Homogeneous Linear Differential Equations
 
Ode powerpoint presentation1
Ode powerpoint presentation1Ode powerpoint presentation1
Ode powerpoint presentation1
 
LINEAR DIFFERENTIAL EQUATION AND BERNOULLIS EQUATIONS
LINEAR DIFFERENTIAL EQUATION AND BERNOULLIS EQUATIONSLINEAR DIFFERENTIAL EQUATION AND BERNOULLIS EQUATIONS
LINEAR DIFFERENTIAL EQUATION AND BERNOULLIS EQUATIONS
 
Ordinary differential equation
Ordinary differential equationOrdinary differential equation
Ordinary differential equation
 
Analytic function
Analytic functionAnalytic function
Analytic function
 
Divergence,curl,gradient
Divergence,curl,gradientDivergence,curl,gradient
Divergence,curl,gradient
 
euler's theorem
euler's theoremeuler's theorem
euler's theorem
 
Complex function
Complex functionComplex function
Complex function
 
introduction to differential equations
introduction to differential equationsintroduction to differential equations
introduction to differential equations
 
Complex function
Complex functionComplex function
Complex function
 
PPT of Improper Integrals IMPROPER INTEGRAL
PPT of Improper Integrals IMPROPER INTEGRALPPT of Improper Integrals IMPROPER INTEGRAL
PPT of Improper Integrals IMPROPER INTEGRAL
 
Fourier integral
Fourier integralFourier integral
Fourier integral
 

Destacado

Lesson 26: The Fundamental Theorem of Calculus (Section 041 slides)
Lesson 26: The Fundamental Theorem of Calculus (Section 041 slides)Lesson 26: The Fundamental Theorem of Calculus (Section 041 slides)
Lesson 26: The Fundamental Theorem of Calculus (Section 041 slides)Matthew Leingang
 
Lesson 26: The Fundamental Theorem of Calculus (Section 021 slides)
Lesson 26: The Fundamental Theorem of Calculus (Section 021 slides)Lesson 26: The Fundamental Theorem of Calculus (Section 021 slides)
Lesson 26: The Fundamental Theorem of Calculus (Section 021 slides)Matthew Leingang
 
Lesson 24: Areas, Distances, the Integral (Section 021 slides)
Lesson 24: Areas, Distances, the Integral (Section 021 slides)Lesson 24: Areas, Distances, the Integral (Section 021 slides)
Lesson 24: Areas, Distances, the Integral (Section 021 slides)Matthew Leingang
 
Lesson 27: Integration by Substitution (Section 041 slides)
Lesson 27: Integration by Substitution (Section 041 slides)Lesson 27: Integration by Substitution (Section 041 slides)
Lesson 27: Integration by Substitution (Section 041 slides)Matthew Leingang
 
Lesson 25: Evaluating Definite Integrals (Section 041 slides)
Lesson 25: Evaluating Definite Integrals (Section 041 slides)Lesson 25: Evaluating Definite Integrals (Section 041 slides)
Lesson 25: Evaluating Definite Integrals (Section 041 slides)Matthew Leingang
 
Lesson 12: Linear Approximations and Differentials (slides)
Lesson 12: Linear Approximations and Differentials (slides)Lesson 12: Linear Approximations and Differentials (slides)
Lesson 12: Linear Approximations and Differentials (slides)Matthew Leingang
 
Lesson 9: The Product and Quotient Rules (slides)
Lesson 9: The Product and Quotient Rules (slides)Lesson 9: The Product and Quotient Rules (slides)
Lesson 9: The Product and Quotient Rules (slides)Matthew Leingang
 
Lesson 2: A Catalog of Essential Functions (slides)
Lesson 2: A Catalog of Essential Functions (slides)Lesson 2: A Catalog of Essential Functions (slides)
Lesson 2: A Catalog of Essential Functions (slides)Matthew Leingang
 
Lesson 1: Functions and their representations (slides)
Lesson 1: Functions and their representations (slides)Lesson 1: Functions and their representations (slides)
Lesson 1: Functions and their representations (slides)Matthew Leingang
 
Lesson 24: Areas, Distances, the Integral (Section 041 slides)
Lesson 24: Areas, Distances, the Integral (Section 041 slides)Lesson 24: Areas, Distances, the Integral (Section 041 slides)
Lesson 24: Areas, Distances, the Integral (Section 041 slides)Matthew Leingang
 

Destacado (13)

Lesson 26: The Fundamental Theorem of Calculus (Section 041 slides)
Lesson 26: The Fundamental Theorem of Calculus (Section 041 slides)Lesson 26: The Fundamental Theorem of Calculus (Section 041 slides)
Lesson 26: The Fundamental Theorem of Calculus (Section 041 slides)
 
Lesson 26: The Fundamental Theorem of Calculus (Section 021 slides)
Lesson 26: The Fundamental Theorem of Calculus (Section 021 slides)Lesson 26: The Fundamental Theorem of Calculus (Section 021 slides)
Lesson 26: The Fundamental Theorem of Calculus (Section 021 slides)
 
Lesson 24: Areas, Distances, the Integral (Section 021 slides)
Lesson 24: Areas, Distances, the Integral (Section 021 slides)Lesson 24: Areas, Distances, the Integral (Section 021 slides)
Lesson 24: Areas, Distances, the Integral (Section 021 slides)
 
Lesson 27: Integration by Substitution (Section 041 slides)
Lesson 27: Integration by Substitution (Section 041 slides)Lesson 27: Integration by Substitution (Section 041 slides)
Lesson 27: Integration by Substitution (Section 041 slides)
 
Lesson 25: Evaluating Definite Integrals (Section 041 slides)
Lesson 25: Evaluating Definite Integrals (Section 041 slides)Lesson 25: Evaluating Definite Integrals (Section 041 slides)
Lesson 25: Evaluating Definite Integrals (Section 041 slides)
 
Lesson 12: Linear Approximations and Differentials (slides)
Lesson 12: Linear Approximations and Differentials (slides)Lesson 12: Linear Approximations and Differentials (slides)
Lesson 12: Linear Approximations and Differentials (slides)
 
Lesson 9: The Product and Quotient Rules (slides)
Lesson 9: The Product and Quotient Rules (slides)Lesson 9: The Product and Quotient Rules (slides)
Lesson 9: The Product and Quotient Rules (slides)
 
Lesson 2: A Catalog of Essential Functions (slides)
Lesson 2: A Catalog of Essential Functions (slides)Lesson 2: A Catalog of Essential Functions (slides)
Lesson 2: A Catalog of Essential Functions (slides)
 
Lesson 1: Functions and their representations (slides)
Lesson 1: Functions and their representations (slides)Lesson 1: Functions and their representations (slides)
Lesson 1: Functions and their representations (slides)
 
Lesson 24: Areas, Distances, the Integral (Section 041 slides)
Lesson 24: Areas, Distances, the Integral (Section 041 slides)Lesson 24: Areas, Distances, the Integral (Section 041 slides)
Lesson 24: Areas, Distances, the Integral (Section 041 slides)
 
Set Theory QA 3
Set Theory QA 3Set Theory QA 3
Set Theory QA 3
 
Permutation and Combination 2
Permutation and Combination 2Permutation and Combination 2
Permutation and Combination 2
 
Wave Motion QA 3
Wave Motion QA 3Wave Motion QA 3
Wave Motion QA 3
 

Similar a Lesson 15: Exponential Growth and Decay (Section 021 slides)

Lesson 15: Exponential Growth and Decay (Section 041 slides)
Lesson 15: Exponential Growth and Decay (Section 041 slides)Lesson 15: Exponential Growth and Decay (Section 041 slides)
Lesson 15: Exponential Growth and Decay (Section 041 slides)Matthew Leingang
 
Lesson 15: Exponential Growth and Decay (Section 021 handout)
Lesson 15: Exponential Growth and Decay (Section 021 handout)Lesson 15: Exponential Growth and Decay (Section 021 handout)
Lesson 15: Exponential Growth and Decay (Section 021 handout)Matthew Leingang
 
Lesson 15: Exponential Growth and Decay (Section 041 handout)
Lesson 15: Exponential Growth and Decay (Section 041 handout)Lesson 15: Exponential Growth and Decay (Section 041 handout)
Lesson 15: Exponential Growth and Decay (Section 041 handout)Matthew Leingang
 
Lesson 15: Exponential Growth and Decay (Section 021 slides)
Lesson 15: Exponential Growth and Decay (Section 021 slides)Lesson 15: Exponential Growth and Decay (Section 021 slides)
Lesson 15: Exponential Growth and Decay (Section 021 slides)Mel Anthony Pepito
 
Lesson15 -exponential_growth_and_decay_021_slides
Lesson15 -exponential_growth_and_decay_021_slidesLesson15 -exponential_growth_and_decay_021_slides
Lesson15 -exponential_growth_and_decay_021_slidesMel Anthony Pepito
 
Lesson 15: Exponential Growth and Decay (Section 041 slides)
Lesson 15: Exponential Growth and Decay (Section 041 slides)Lesson 15: Exponential Growth and Decay (Section 041 slides)
Lesson 15: Exponential Growth and Decay (Section 041 slides)Mel Anthony Pepito
 
Lesson 15: Exponential Growth and Decay
Lesson 15: Exponential Growth and DecayLesson 15: Exponential Growth and Decay
Lesson 15: Exponential Growth and DecayMel Anthony Pepito
 
Lesson 15: Exponential Growth and Decay
Lesson 15: Exponential Growth and DecayLesson 15: Exponential Growth and Decay
Lesson 15: Exponential Growth and DecayMatthew Leingang
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Matthew Leingang
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Matthew Leingang
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Matthew Leingang
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Matthew Leingang
 
Lesson 20: Derivatives and the Shape of Curves (Section 041 slides)
Lesson 20: Derivatives and the Shape of Curves (Section 041 slides)Lesson 20: Derivatives and the Shape of Curves (Section 041 slides)
Lesson 20: Derivatives and the Shape of Curves (Section 041 slides)Matthew Leingang
 
Lesson 14: Exponential Growth and Decay
Lesson 14: Exponential Growth and DecayLesson 14: Exponential Growth and Decay
Lesson 14: Exponential Growth and DecayMatthew Leingang
 
Lesson 15: Exponential Growth and Decay (handout)
Lesson 15: Exponential Growth and Decay (handout)Lesson 15: Exponential Growth and Decay (handout)
Lesson 15: Exponential Growth and Decay (handout)Matthew Leingang
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Mel Anthony Pepito
 
Lesson20 -derivatives_and_the_shape_of_curves_021_slides
Lesson20  -derivatives_and_the_shape_of_curves_021_slidesLesson20  -derivatives_and_the_shape_of_curves_021_slides
Lesson20 -derivatives_and_the_shape_of_curves_021_slidesMatthew Leingang
 
Lesson 21: Antiderivatives (slides)
Lesson 21: Antiderivatives (slides)Lesson 21: Antiderivatives (slides)
Lesson 21: Antiderivatives (slides)Matthew Leingang
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Mel Anthony Pepito
 
Lesson 23: Antiderivatives (Section 021 handout)
Lesson 23: Antiderivatives (Section 021 handout)Lesson 23: Antiderivatives (Section 021 handout)
Lesson 23: Antiderivatives (Section 021 handout)Matthew Leingang
 

Similar a Lesson 15: Exponential Growth and Decay (Section 021 slides) (20)

Lesson 15: Exponential Growth and Decay (Section 041 slides)
Lesson 15: Exponential Growth and Decay (Section 041 slides)Lesson 15: Exponential Growth and Decay (Section 041 slides)
Lesson 15: Exponential Growth and Decay (Section 041 slides)
 
Lesson 15: Exponential Growth and Decay (Section 021 handout)
Lesson 15: Exponential Growth and Decay (Section 021 handout)Lesson 15: Exponential Growth and Decay (Section 021 handout)
Lesson 15: Exponential Growth and Decay (Section 021 handout)
 
Lesson 15: Exponential Growth and Decay (Section 041 handout)
Lesson 15: Exponential Growth and Decay (Section 041 handout)Lesson 15: Exponential Growth and Decay (Section 041 handout)
Lesson 15: Exponential Growth and Decay (Section 041 handout)
 
Lesson 15: Exponential Growth and Decay (Section 021 slides)
Lesson 15: Exponential Growth and Decay (Section 021 slides)Lesson 15: Exponential Growth and Decay (Section 021 slides)
Lesson 15: Exponential Growth and Decay (Section 021 slides)
 
Lesson15 -exponential_growth_and_decay_021_slides
Lesson15 -exponential_growth_and_decay_021_slidesLesson15 -exponential_growth_and_decay_021_slides
Lesson15 -exponential_growth_and_decay_021_slides
 
Lesson 15: Exponential Growth and Decay (Section 041 slides)
Lesson 15: Exponential Growth and Decay (Section 041 slides)Lesson 15: Exponential Growth and Decay (Section 041 slides)
Lesson 15: Exponential Growth and Decay (Section 041 slides)
 
Lesson 15: Exponential Growth and Decay
Lesson 15: Exponential Growth and DecayLesson 15: Exponential Growth and Decay
Lesson 15: Exponential Growth and Decay
 
Lesson 15: Exponential Growth and Decay
Lesson 15: Exponential Growth and DecayLesson 15: Exponential Growth and Decay
Lesson 15: Exponential Growth and Decay
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
 
Lesson 20: Derivatives and the Shape of Curves (Section 041 slides)
Lesson 20: Derivatives and the Shape of Curves (Section 041 slides)Lesson 20: Derivatives and the Shape of Curves (Section 041 slides)
Lesson 20: Derivatives and the Shape of Curves (Section 041 slides)
 
Lesson 14: Exponential Growth and Decay
Lesson 14: Exponential Growth and DecayLesson 14: Exponential Growth and Decay
Lesson 14: Exponential Growth and Decay
 
Lesson 15: Exponential Growth and Decay (handout)
Lesson 15: Exponential Growth and Decay (handout)Lesson 15: Exponential Growth and Decay (handout)
Lesson 15: Exponential Growth and Decay (handout)
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 021 ...
 
Lesson20 -derivatives_and_the_shape_of_curves_021_slides
Lesson20  -derivatives_and_the_shape_of_curves_021_slidesLesson20  -derivatives_and_the_shape_of_curves_021_slides
Lesson20 -derivatives_and_the_shape_of_curves_021_slides
 
Lesson 21: Antiderivatives (slides)
Lesson 21: Antiderivatives (slides)Lesson 21: Antiderivatives (slides)
Lesson 21: Antiderivatives (slides)
 
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
Lesson 14: Derivatives of Exponential and Logarithmic Functions (Section 041 ...
 
Lesson 23: Antiderivatives (Section 021 handout)
Lesson 23: Antiderivatives (Section 021 handout)Lesson 23: Antiderivatives (Section 021 handout)
Lesson 23: Antiderivatives (Section 021 handout)
 

Más de Matthew Leingang

Streamlining assessment, feedback, and archival with auto-multiple-choice
Streamlining assessment, feedback, and archival with auto-multiple-choiceStreamlining assessment, feedback, and archival with auto-multiple-choice
Streamlining assessment, feedback, and archival with auto-multiple-choiceMatthew Leingang
 
Electronic Grading of Paper Assessments
Electronic Grading of Paper AssessmentsElectronic Grading of Paper Assessments
Electronic Grading of Paper AssessmentsMatthew Leingang
 
Lesson 27: Integration by Substitution (slides)
Lesson 27: Integration by Substitution (slides)Lesson 27: Integration by Substitution (slides)
Lesson 27: Integration by Substitution (slides)Matthew Leingang
 
Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)Matthew Leingang
 
Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)Matthew Leingang
 
Lesson 27: Integration by Substitution (handout)
Lesson 27: Integration by Substitution (handout)Lesson 27: Integration by Substitution (handout)
Lesson 27: Integration by Substitution (handout)Matthew Leingang
 
Lesson 26: The Fundamental Theorem of Calculus (handout)
Lesson 26: The Fundamental Theorem of Calculus (handout)Lesson 26: The Fundamental Theorem of Calculus (handout)
Lesson 26: The Fundamental Theorem of Calculus (handout)Matthew Leingang
 
Lesson 25: Evaluating Definite Integrals (slides)
Lesson 25: Evaluating Definite Integrals (slides)Lesson 25: Evaluating Definite Integrals (slides)
Lesson 25: Evaluating Definite Integrals (slides)Matthew Leingang
 
Lesson 25: Evaluating Definite Integrals (handout)
Lesson 25: Evaluating Definite Integrals (handout)Lesson 25: Evaluating Definite Integrals (handout)
Lesson 25: Evaluating Definite Integrals (handout)Matthew Leingang
 
Lesson 24: Areas and Distances, The Definite Integral (handout)
Lesson 24: Areas and Distances, The Definite Integral (handout)Lesson 24: Areas and Distances, The Definite Integral (handout)
Lesson 24: Areas and Distances, The Definite Integral (handout)Matthew Leingang
 
Lesson 24: Areas and Distances, The Definite Integral (slides)
Lesson 24: Areas and Distances, The Definite Integral (slides)Lesson 24: Areas and Distances, The Definite Integral (slides)
Lesson 24: Areas and Distances, The Definite Integral (slides)Matthew Leingang
 
Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)Matthew Leingang
 
Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)Matthew Leingang
 
Lesson 22: Optimization Problems (slides)
Lesson 22: Optimization Problems (slides)Lesson 22: Optimization Problems (slides)
Lesson 22: Optimization Problems (slides)Matthew Leingang
 
Lesson 22: Optimization Problems (handout)
Lesson 22: Optimization Problems (handout)Lesson 22: Optimization Problems (handout)
Lesson 22: Optimization Problems (handout)Matthew Leingang
 
Lesson 21: Curve Sketching (slides)
Lesson 21: Curve Sketching (slides)Lesson 21: Curve Sketching (slides)
Lesson 21: Curve Sketching (slides)Matthew Leingang
 
Lesson 21: Curve Sketching (handout)
Lesson 21: Curve Sketching (handout)Lesson 21: Curve Sketching (handout)
Lesson 21: Curve Sketching (handout)Matthew Leingang
 
Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)Matthew Leingang
 
Lesson 20: Derivatives and the Shapes of Curves (handout)
Lesson 20: Derivatives and the Shapes of Curves (handout)Lesson 20: Derivatives and the Shapes of Curves (handout)
Lesson 20: Derivatives and the Shapes of Curves (handout)Matthew Leingang
 

Más de Matthew Leingang (20)

Making Lesson Plans
Making Lesson PlansMaking Lesson Plans
Making Lesson Plans
 
Streamlining assessment, feedback, and archival with auto-multiple-choice
Streamlining assessment, feedback, and archival with auto-multiple-choiceStreamlining assessment, feedback, and archival with auto-multiple-choice
Streamlining assessment, feedback, and archival with auto-multiple-choice
 
Electronic Grading of Paper Assessments
Electronic Grading of Paper AssessmentsElectronic Grading of Paper Assessments
Electronic Grading of Paper Assessments
 
Lesson 27: Integration by Substitution (slides)
Lesson 27: Integration by Substitution (slides)Lesson 27: Integration by Substitution (slides)
Lesson 27: Integration by Substitution (slides)
 
Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)
 
Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)Lesson 26: The Fundamental Theorem of Calculus (slides)
Lesson 26: The Fundamental Theorem of Calculus (slides)
 
Lesson 27: Integration by Substitution (handout)
Lesson 27: Integration by Substitution (handout)Lesson 27: Integration by Substitution (handout)
Lesson 27: Integration by Substitution (handout)
 
Lesson 26: The Fundamental Theorem of Calculus (handout)
Lesson 26: The Fundamental Theorem of Calculus (handout)Lesson 26: The Fundamental Theorem of Calculus (handout)
Lesson 26: The Fundamental Theorem of Calculus (handout)
 
Lesson 25: Evaluating Definite Integrals (slides)
Lesson 25: Evaluating Definite Integrals (slides)Lesson 25: Evaluating Definite Integrals (slides)
Lesson 25: Evaluating Definite Integrals (slides)
 
Lesson 25: Evaluating Definite Integrals (handout)
Lesson 25: Evaluating Definite Integrals (handout)Lesson 25: Evaluating Definite Integrals (handout)
Lesson 25: Evaluating Definite Integrals (handout)
 
Lesson 24: Areas and Distances, The Definite Integral (handout)
Lesson 24: Areas and Distances, The Definite Integral (handout)Lesson 24: Areas and Distances, The Definite Integral (handout)
Lesson 24: Areas and Distances, The Definite Integral (handout)
 
Lesson 24: Areas and Distances, The Definite Integral (slides)
Lesson 24: Areas and Distances, The Definite Integral (slides)Lesson 24: Areas and Distances, The Definite Integral (slides)
Lesson 24: Areas and Distances, The Definite Integral (slides)
 
Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)
 
Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)Lesson 23: Antiderivatives (slides)
Lesson 23: Antiderivatives (slides)
 
Lesson 22: Optimization Problems (slides)
Lesson 22: Optimization Problems (slides)Lesson 22: Optimization Problems (slides)
Lesson 22: Optimization Problems (slides)
 
Lesson 22: Optimization Problems (handout)
Lesson 22: Optimization Problems (handout)Lesson 22: Optimization Problems (handout)
Lesson 22: Optimization Problems (handout)
 
Lesson 21: Curve Sketching (slides)
Lesson 21: Curve Sketching (slides)Lesson 21: Curve Sketching (slides)
Lesson 21: Curve Sketching (slides)
 
Lesson 21: Curve Sketching (handout)
Lesson 21: Curve Sketching (handout)Lesson 21: Curve Sketching (handout)
Lesson 21: Curve Sketching (handout)
 
Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)Lesson 20: Derivatives and the Shapes of Curves (slides)
Lesson 20: Derivatives and the Shapes of Curves (slides)
 
Lesson 20: Derivatives and the Shapes of Curves (handout)
Lesson 20: Derivatives and the Shapes of Curves (handout)Lesson 20: Derivatives and the Shapes of Curves (handout)
Lesson 20: Derivatives and the Shapes of Curves (handout)
 

Último

SAP Build Work Zone - Overview L2-L3.pptx
SAP Build Work Zone - Overview L2-L3.pptxSAP Build Work Zone - Overview L2-L3.pptx
SAP Build Work Zone - Overview L2-L3.pptxNavinnSomaal
 
Anypoint Exchange: It’s Not Just a Repo!
Anypoint Exchange: It’s Not Just a Repo!Anypoint Exchange: It’s Not Just a Repo!
Anypoint Exchange: It’s Not Just a Repo!Manik S Magar
 
Nell’iperspazio con Rocket: il Framework Web di Rust!
Nell’iperspazio con Rocket: il Framework Web di Rust!Nell’iperspazio con Rocket: il Framework Web di Rust!
Nell’iperspazio con Rocket: il Framework Web di Rust!Commit University
 
Vector Databases 101 - An introduction to the world of Vector Databases
Vector Databases 101 - An introduction to the world of Vector DatabasesVector Databases 101 - An introduction to the world of Vector Databases
Vector Databases 101 - An introduction to the world of Vector DatabasesZilliz
 
Vertex AI Gemini Prompt Engineering Tips
Vertex AI Gemini Prompt Engineering TipsVertex AI Gemini Prompt Engineering Tips
Vertex AI Gemini Prompt Engineering TipsMiki Katsuragi
 
"Federated learning: out of reach no matter how close",Oleksandr Lapshyn
"Federated learning: out of reach no matter how close",Oleksandr Lapshyn"Federated learning: out of reach no matter how close",Oleksandr Lapshyn
"Federated learning: out of reach no matter how close",Oleksandr LapshynFwdays
 
"Debugging python applications inside k8s environment", Andrii Soldatenko
"Debugging python applications inside k8s environment", Andrii Soldatenko"Debugging python applications inside k8s environment", Andrii Soldatenko
"Debugging python applications inside k8s environment", Andrii SoldatenkoFwdays
 
Unraveling Multimodality with Large Language Models.pdf
Unraveling Multimodality with Large Language Models.pdfUnraveling Multimodality with Large Language Models.pdf
Unraveling Multimodality with Large Language Models.pdfAlex Barbosa Coqueiro
 
DevoxxFR 2024 Reproducible Builds with Apache Maven
DevoxxFR 2024 Reproducible Builds with Apache MavenDevoxxFR 2024 Reproducible Builds with Apache Maven
DevoxxFR 2024 Reproducible Builds with Apache MavenHervé Boutemy
 
The Future of Software Development - Devin AI Innovative Approach.pdf
The Future of Software Development - Devin AI Innovative Approach.pdfThe Future of Software Development - Devin AI Innovative Approach.pdf
The Future of Software Development - Devin AI Innovative Approach.pdfSeasiaInfotech2
 
My INSURER PTE LTD - Insurtech Innovation Award 2024
My INSURER PTE LTD - Insurtech Innovation Award 2024My INSURER PTE LTD - Insurtech Innovation Award 2024
My INSURER PTE LTD - Insurtech Innovation Award 2024The Digital Insurer
 
Artificial intelligence in cctv survelliance.pptx
Artificial intelligence in cctv survelliance.pptxArtificial intelligence in cctv survelliance.pptx
Artificial intelligence in cctv survelliance.pptxhariprasad279825
 
New from BookNet Canada for 2024: BNC CataList - Tech Forum 2024
New from BookNet Canada for 2024: BNC CataList - Tech Forum 2024New from BookNet Canada for 2024: BNC CataList - Tech Forum 2024
New from BookNet Canada for 2024: BNC CataList - Tech Forum 2024BookNet Canada
 
AI as an Interface for Commercial Buildings
AI as an Interface for Commercial BuildingsAI as an Interface for Commercial Buildings
AI as an Interface for Commercial BuildingsMemoori
 
Story boards and shot lists for my a level piece
Story boards and shot lists for my a level pieceStory boards and shot lists for my a level piece
Story boards and shot lists for my a level piececharlottematthew16
 
My Hashitalk Indonesia April 2024 Presentation
My Hashitalk Indonesia April 2024 PresentationMy Hashitalk Indonesia April 2024 Presentation
My Hashitalk Indonesia April 2024 PresentationRidwan Fadjar
 
Dev Dives: Streamline document processing with UiPath Studio Web
Dev Dives: Streamline document processing with UiPath Studio WebDev Dives: Streamline document processing with UiPath Studio Web
Dev Dives: Streamline document processing with UiPath Studio WebUiPathCommunity
 
Install Stable Diffusion in windows machine
Install Stable Diffusion in windows machineInstall Stable Diffusion in windows machine
Install Stable Diffusion in windows machinePadma Pradeep
 

Último (20)

SAP Build Work Zone - Overview L2-L3.pptx
SAP Build Work Zone - Overview L2-L3.pptxSAP Build Work Zone - Overview L2-L3.pptx
SAP Build Work Zone - Overview L2-L3.pptx
 
DMCC Future of Trade Web3 - Special Edition
DMCC Future of Trade Web3 - Special EditionDMCC Future of Trade Web3 - Special Edition
DMCC Future of Trade Web3 - Special Edition
 
Anypoint Exchange: It’s Not Just a Repo!
Anypoint Exchange: It’s Not Just a Repo!Anypoint Exchange: It’s Not Just a Repo!
Anypoint Exchange: It’s Not Just a Repo!
 
Nell’iperspazio con Rocket: il Framework Web di Rust!
Nell’iperspazio con Rocket: il Framework Web di Rust!Nell’iperspazio con Rocket: il Framework Web di Rust!
Nell’iperspazio con Rocket: il Framework Web di Rust!
 
Vector Databases 101 - An introduction to the world of Vector Databases
Vector Databases 101 - An introduction to the world of Vector DatabasesVector Databases 101 - An introduction to the world of Vector Databases
Vector Databases 101 - An introduction to the world of Vector Databases
 
Vertex AI Gemini Prompt Engineering Tips
Vertex AI Gemini Prompt Engineering TipsVertex AI Gemini Prompt Engineering Tips
Vertex AI Gemini Prompt Engineering Tips
 
"Federated learning: out of reach no matter how close",Oleksandr Lapshyn
"Federated learning: out of reach no matter how close",Oleksandr Lapshyn"Federated learning: out of reach no matter how close",Oleksandr Lapshyn
"Federated learning: out of reach no matter how close",Oleksandr Lapshyn
 
"Debugging python applications inside k8s environment", Andrii Soldatenko
"Debugging python applications inside k8s environment", Andrii Soldatenko"Debugging python applications inside k8s environment", Andrii Soldatenko
"Debugging python applications inside k8s environment", Andrii Soldatenko
 
Unraveling Multimodality with Large Language Models.pdf
Unraveling Multimodality with Large Language Models.pdfUnraveling Multimodality with Large Language Models.pdf
Unraveling Multimodality with Large Language Models.pdf
 
DevoxxFR 2024 Reproducible Builds with Apache Maven
DevoxxFR 2024 Reproducible Builds with Apache MavenDevoxxFR 2024 Reproducible Builds with Apache Maven
DevoxxFR 2024 Reproducible Builds with Apache Maven
 
E-Vehicle_Hacking_by_Parul Sharma_null_owasp.pptx
E-Vehicle_Hacking_by_Parul Sharma_null_owasp.pptxE-Vehicle_Hacking_by_Parul Sharma_null_owasp.pptx
E-Vehicle_Hacking_by_Parul Sharma_null_owasp.pptx
 
The Future of Software Development - Devin AI Innovative Approach.pdf
The Future of Software Development - Devin AI Innovative Approach.pdfThe Future of Software Development - Devin AI Innovative Approach.pdf
The Future of Software Development - Devin AI Innovative Approach.pdf
 
My INSURER PTE LTD - Insurtech Innovation Award 2024
My INSURER PTE LTD - Insurtech Innovation Award 2024My INSURER PTE LTD - Insurtech Innovation Award 2024
My INSURER PTE LTD - Insurtech Innovation Award 2024
 
Artificial intelligence in cctv survelliance.pptx
Artificial intelligence in cctv survelliance.pptxArtificial intelligence in cctv survelliance.pptx
Artificial intelligence in cctv survelliance.pptx
 
New from BookNet Canada for 2024: BNC CataList - Tech Forum 2024
New from BookNet Canada for 2024: BNC CataList - Tech Forum 2024New from BookNet Canada for 2024: BNC CataList - Tech Forum 2024
New from BookNet Canada for 2024: BNC CataList - Tech Forum 2024
 
AI as an Interface for Commercial Buildings
AI as an Interface for Commercial BuildingsAI as an Interface for Commercial Buildings
AI as an Interface for Commercial Buildings
 
Story boards and shot lists for my a level piece
Story boards and shot lists for my a level pieceStory boards and shot lists for my a level piece
Story boards and shot lists for my a level piece
 
My Hashitalk Indonesia April 2024 Presentation
My Hashitalk Indonesia April 2024 PresentationMy Hashitalk Indonesia April 2024 Presentation
My Hashitalk Indonesia April 2024 Presentation
 
Dev Dives: Streamline document processing with UiPath Studio Web
Dev Dives: Streamline document processing with UiPath Studio WebDev Dives: Streamline document processing with UiPath Studio Web
Dev Dives: Streamline document processing with UiPath Studio Web
 
Install Stable Diffusion in windows machine
Install Stable Diffusion in windows machineInstall Stable Diffusion in windows machine
Install Stable Diffusion in windows machine
 

Lesson 15: Exponential Growth and Decay (Section 021 slides)

  • 1. Section 3.4 Exponential Growth and Decay V63.0121.021, Calculus I New York University October 28, 2010 Announcements Quiz 3 next week in recitation on 2.6, 2.8, 3.1, 3.2 . . . . . .
  • 2. . . . . . . Announcements Quiz 3 next week in recitation on 2.6, 2.8, 3.1, 3.2 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 2 / 40
  • 3. . . . . . . Objectives Solve the ordinary differential equation y′ (t) = ky(t), y(0) = y0 Solve problems involving exponential growth and decay V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 3 / 40
  • 4. . . . . . . Outline Recall The differential equation y′ = ky Modeling simple population growth Modeling radioactive decay Carbon-14 Dating Newton’s Law of Cooling Continuously Compounded Interest V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 4 / 40
  • 5. . . . . . . Derivatives of exponential and logarithmic functions y y′ ex ex ax (ln a) · ax ln x 1 x loga x 1 ln a · 1 x V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 5 / 40
  • 6. . . . . . . Outline Recall The differential equation y′ = ky Modeling simple population growth Modeling radioactive decay Carbon-14 Dating Newton’s Law of Cooling Continuously Compounded Interest V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 6 / 40
  • 7. . . . . . . What is a differential equation? Definition A differential equation is an equation for an unknown function which includes the function and its derivatives. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 7 / 40
  • 8. . . . . . . What is a differential equation? Definition A differential equation is an equation for an unknown function which includes the function and its derivatives. Example Newton’s Second Law F = ma is a differential equation, where a(t) = x′′ (t). V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 7 / 40
  • 9. . . . . . . What is a differential equation? Definition A differential equation is an equation for an unknown function which includes the function and its derivatives. Example Newton’s Second Law F = ma is a differential equation, where a(t) = x′′ (t). In a spring, F(x) = −kx, where x is displacement from equilibrium and k is a constant. So −kx(t) = mx′′ (t) =⇒ x′′ (t) + k m x(t) = 0. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 7 / 40
  • 10. . . . . . . What is a differential equation? Definition A differential equation is an equation for an unknown function which includes the function and its derivatives. Example Newton’s Second Law F = ma is a differential equation, where a(t) = x′′ (t). In a spring, F(x) = −kx, where x is displacement from equilibrium and k is a constant. So −kx(t) = mx′′ (t) =⇒ x′′ (t) + k m x(t) = 0. The most general solution is x(t) = A sin ωt + B cos ωt, where ω = √ k/m. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 7 / 40
  • 11. . . . . . . Showing a function is a solution Example (Continued) Show that x(t) = A sin ωt + B cos ωt satisfies the differential equation x′′ + k m x = 0, where ω = √ k/m. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 8 / 40
  • 12. . . . . . . Showing a function is a solution Example (Continued) Show that x(t) = A sin ωt + B cos ωt satisfies the differential equation x′′ + k m x = 0, where ω = √ k/m. Solution We have x(t) = A sin ωt + B cos ωt x′ (t) = Aω cos ωt − Bω sin ωt x′′ (t) = −Aω2 sin ωt − Bω2 cos ωt Since ω2 = k/m, the last line plus k/m times the first line result in zero. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 8 / 40
  • 13. . . . . . . The Equation y′ = 2 Example Find a solution to y′ (t) = 2. Find the most general solution to y′ (t) = 2. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 9 / 40
  • 14. . . . . . . The Equation y′ = 2 Example Find a solution to y′ (t) = 2. Find the most general solution to y′ (t) = 2. Solution A solution is y(t) = 2t. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 9 / 40
  • 15. . . . . . . The Equation y′ = 2 Example Find a solution to y′ (t) = 2. Find the most general solution to y′ (t) = 2. Solution A solution is y(t) = 2t. The general solution is y = 2t + C. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 9 / 40
  • 16. . . . . . . The Equation y′ = 2 Example Find a solution to y′ (t) = 2. Find the most general solution to y′ (t) = 2. Solution A solution is y(t) = 2t. The general solution is y = 2t + C. Remark If a function has a constant rate of growth, it’s linear. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 9 / 40
  • 17. . . . . . . The Equation y′ = 2t Example Find a solution to y′ (t) = 2t. Find the most general solution to y′ (t) = 2t. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 10 / 40
  • 18. . . . . . . The Equation y′ = 2t Example Find a solution to y′ (t) = 2t. Find the most general solution to y′ (t) = 2t. Solution A solution is y(t) = t2 . V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 10 / 40
  • 19. . . . . . . The Equation y′ = 2t Example Find a solution to y′ (t) = 2t. Find the most general solution to y′ (t) = 2t. Solution A solution is y(t) = t2 . The general solution is y = t2 + C. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 10 / 40
  • 20. . . . . . . The Equation y′ = y Example Find a solution to y′ (t) = y(t). Find the most general solution to y′ (t) = y(t). V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 11 / 40
  • 21. . . . . . . The Equation y′ = y Example Find a solution to y′ (t) = y(t). Find the most general solution to y′ (t) = y(t). Solution A solution is y(t) = et . V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 11 / 40
  • 22. . . . . . . The Equation y′ = y Example Find a solution to y′ (t) = y(t). Find the most general solution to y′ (t) = y(t). Solution A solution is y(t) = et . The general solution is y = Cet , not y = et + C. (check this) V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 11 / 40
  • 23. . . . . . . Kick it up a notch: y′ = 2y Example Find a solution to y′ = 2y. Find the general solution to y′ = 2y. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 12 / 40
  • 24. . . . . . . Kick it up a notch: y′ = 2y Example Find a solution to y′ = 2y. Find the general solution to y′ = 2y. Solution y = e2t y = Ce2t V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 12 / 40
  • 25. . . . . . . In general: y′ = ky Example Find a solution to y′ = ky. Find the general solution to y′ = ky. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 13 / 40
  • 26. . . . . . . In general: y′ = ky Example Find a solution to y′ = ky. Find the general solution to y′ = ky. Solution y = ekt y = Cekt V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 13 / 40
  • 27. . . . . . . In general: y′ = ky Example Find a solution to y′ = ky. Find the general solution to y′ = ky. Solution y = ekt y = Cekt Remark What is C? Plug in t = 0: y(0) = Cek·0 = C · 1 = C, so y(0) = y0, the initial value of y. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 13 / 40
  • 28. . . . . . . Constant Relative Growth =⇒ Exponential Growth Theorem A function with constant relative growth rate k is an exponential function with parameter k. Explicitly, the solution to the equation y′ (t) = ky(t) y(0) = y0 is y(t) = y0ekt V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 14 / 40
  • 29. . . . . . . Exponential Growth is everywhere Lots of situations have growth rates proportional to the current value This is the same as saying the relative growth rate is constant. Examples: Natural population growth, compounded interest, social networks V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 15 / 40
  • 30. . . . . . . Outline Recall The differential equation y′ = ky Modeling simple population growth Modeling radioactive decay Carbon-14 Dating Newton’s Law of Cooling Continuously Compounded Interest V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 16 / 40
  • 31. . . . . . . Bacteria Since you need bacteria to make bacteria, the amount of new bacteria at any moment is proportional to the total amount of bacteria. This means bacteria populations grow exponentially. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 17 / 40
  • 32. . . . . . . Bacteria Example Example A colony of bacteria is grown under ideal conditions in a laboratory. At the end of 3 hours there are 10,000 bacteria. At the end of 5 hours there are 40,000. How many bacteria were present initially? V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 18 / 40
  • 33. . . . . . . Bacteria Example Example A colony of bacteria is grown under ideal conditions in a laboratory. At the end of 3 hours there are 10,000 bacteria. At the end of 5 hours there are 40,000. How many bacteria were present initially? Solution Since y′ = ky for bacteria, we have y = y0ekt . We have 10, 000 = y0ek·3 40, 000 = y0ek·5 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 18 / 40
  • 34. . . . . . . Bacteria Example Example A colony of bacteria is grown under ideal conditions in a laboratory. At the end of 3 hours there are 10,000 bacteria. At the end of 5 hours there are 40,000. How many bacteria were present initially? Solution Since y′ = ky for bacteria, we have y = y0ekt . We have 10, 000 = y0ek·3 40, 000 = y0ek·5 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 18 / 40
  • 35. . . . . . . Bacteria Example Example A colony of bacteria is grown under ideal conditions in a laboratory. At the end of 3 hours there are 10,000 bacteria. At the end of 5 hours there are 40,000. How many bacteria were present initially? Solution Since y′ = ky for bacteria, we have y = y0ekt . We have 10, 000 = y0ek·3 40, 000 = y0ek·5 Dividing the first into the second gives 4 = e2k =⇒ 2k = ln 4 =⇒ k = ln 2. Now we have 10, 000 = y0eln 2·3 = y0 · 8 So y0 = 10, 000 8 = 1250. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 18 / 40
  • 36. . . . . . . Could you do that again please? We have 10, 000 = y0ek·3 40, 000 = y0ek·5 Dividing the first into the second gives 40, 000 10, 000 = y0e5k y0e3k =⇒ 4 = e2k =⇒ ln 4 = ln(e2k ) = 2k =⇒ k = ln 4 2 = ln 22 2 = 2 ln 2 2 = ln 2 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 19 / 40
  • 37. . . . . . . Outline Recall The differential equation y′ = ky Modeling simple population growth Modeling radioactive decay Carbon-14 Dating Newton’s Law of Cooling Continuously Compounded Interest V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 20 / 40
  • 38. . . . . . . Modeling radioactive decay Radioactive decay occurs because many large atoms spontaneously give off particles. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 21 / 40
  • 39. . . . . . . Modeling radioactive decay Radioactive decay occurs because many large atoms spontaneously give off particles. This means that in a sample of a bunch of atoms, we can assume a certain percentage of them will “go off” at any point. (For instance, if all atom of a certain radioactive element have a 20% chance of decaying at any point, then we can expect in a sample of 100 that 20 of them will be decaying.) V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 21 / 40
  • 40. . . . . . . Radioactive decay as a differential equation The relative rate of decay is constant: y′ y = k where k is negative. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 22 / 40
  • 41. . . . . . . Radioactive decay as a differential equation The relative rate of decay is constant: y′ y = k where k is negative. So y′ = ky =⇒ y = y0ekt again! V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 22 / 40
  • 42. . . . . . . Radioactive decay as a differential equation The relative rate of decay is constant: y′ y = k where k is negative. So y′ = ky =⇒ y = y0ekt again! It’s customary to express the relative rate of decay in the units of half-life: the amount of time it takes a pure sample to decay to one which is only half pure. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 22 / 40
  • 43. . . . . . . Computing the amount remaining of a decaying sample Example The half-life of polonium-210 is about 138 days. How much of a 100 g sample remains after t years? V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 23 / 40
  • 44. . . . . . . Computing the amount remaining of a decaying sample Example The half-life of polonium-210 is about 138 days. How much of a 100 g sample remains after t years? Solution We have y = y0ekt , where y0 = y(0) = 100 grams. Then 50 = 100ek·138/365 =⇒ k = − 365 · ln 2 138 . Therefore y(t) = 100e−365·ln 2 138 t = 100 · 2−365t/138 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 23 / 40
  • 45. . . . . . . Computing the amount remaining of a decaying sample Example The half-life of polonium-210 is about 138 days. How much of a 100 g sample remains after t years? Solution We have y = y0ekt , where y0 = y(0) = 100 grams. Then 50 = 100ek·138/365 =⇒ k = − 365 · ln 2 138 . Therefore y(t) = 100e−365·ln 2 138 t = 100 · 2−365t/138 Notice y(t) = y0 · 2−t/t1/2 , where t1/2 is the half-life. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 23 / 40
  • 46. . . . . . . Carbon-14 Dating The ratio of carbon-14 to carbon-12 in an organism decays exponentially: p(t) = p0e−kt . The half-life of carbon-14 is about 5700 years. So the equation for p(t) is p(t) = p0e− ln2 5700 t Another way to write this would be p(t) = p02−t/5700 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 24 / 40
  • 47. . . . . . . Computing age with Carbon-14 content Example Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is 10% of that in a living organism. How old is the fossil? V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
  • 48. . . . . . . Computing age with Carbon-14 content Example Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is 10% of that in a living organism. How old is the fossil? Solution We are looking for the value of t for which p(t) p0 = 0.1 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
  • 49. . . . . . . Computing age with Carbon-14 content Example Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is 10% of that in a living organism. How old is the fossil? Solution We are looking for the value of t for which p(t) p0 = 0.1 From the equation we have 2−t/5700 = 0.1 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
  • 50. . . . . . . Computing age with Carbon-14 content Example Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is 10% of that in a living organism. How old is the fossil? Solution We are looking for the value of t for which p(t) p0 = 0.1 From the equation we have 2−t/5700 = 0.1 =⇒ − t 5700 ln 2 = ln 0.1 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
  • 51. . . . . . . Computing age with Carbon-14 content Example Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is 10% of that in a living organism. How old is the fossil? Solution We are looking for the value of t for which p(t) p0 = 0.1 From the equation we have 2−t/5700 = 0.1 =⇒ − t 5700 ln 2 = ln 0.1 =⇒ t = ln 0.1 ln 2 · 5700 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
  • 52. . . . . . . Computing age with Carbon-14 content Example Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is 10% of that in a living organism. How old is the fossil? Solution We are looking for the value of t for which p(t) p0 = 0.1 From the equation we have 2−t/5700 = 0.1 =⇒ − t 5700 ln 2 = ln 0.1 =⇒ t = ln 0.1 ln 2 · 5700 ≈ 18, 940 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
  • 53. . . . . . . Computing age with Carbon-14 content Example Suppose a fossil is found where the ratio of carbon-14 to carbon-12 is 10% of that in a living organism. How old is the fossil? Solution We are looking for the value of t for which p(t) p0 = 0.1 From the equation we have 2−t/5700 = 0.1 =⇒ − t 5700 ln 2 = ln 0.1 =⇒ t = ln 0.1 ln 2 · 5700 ≈ 18, 940 So the fossil is almost 19,000 years old. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 25 / 40
  • 54. . . . . . . Outline Recall The differential equation y′ = ky Modeling simple population growth Modeling radioactive decay Carbon-14 Dating Newton’s Law of Cooling Continuously Compounded Interest V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 26 / 40
  • 55. . . . . . . Newton's Law of Cooling Newton’s Law of Cooling states that the rate of cooling of an object is proportional to the temperature difference between the object and its surroundings. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 27 / 40
  • 56. . . . . . . Newton's Law of Cooling Newton’s Law of Cooling states that the rate of cooling of an object is proportional to the temperature difference between the object and its surroundings. This gives us a differential equation of the form dT dt = k(T − Ts) (where k < 0 again). V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 27 / 40
  • 57. . . . . . . General Solution to NLC problems To solve this, change the variable y(t) = T(t) − Ts. Then y′ = T′ and k(T − Ts) = ky. The equation now looks like dT dt = k(T − Ts) ⇐⇒ dy dt = ky V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
  • 58. . . . . . . General Solution to NLC problems To solve this, change the variable y(t) = T(t) − Ts. Then y′ = T′ and k(T − Ts) = ky. The equation now looks like dT dt = k(T − Ts) ⇐⇒ dy dt = ky Now we can solve! y′ = ky V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
  • 59. . . . . . . General Solution to NLC problems To solve this, change the variable y(t) = T(t) − Ts. Then y′ = T′ and k(T − Ts) = ky. The equation now looks like dT dt = k(T − Ts) ⇐⇒ dy dt = ky Now we can solve! y′ = ky =⇒ y = Cekt V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
  • 60. . . . . . . General Solution to NLC problems To solve this, change the variable y(t) = T(t) − Ts. Then y′ = T′ and k(T − Ts) = ky. The equation now looks like dT dt = k(T − Ts) ⇐⇒ dy dt = ky Now we can solve! y′ = ky =⇒ y = Cekt =⇒ T − Ts = Cekt V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
  • 61. . . . . . . General Solution to NLC problems To solve this, change the variable y(t) = T(t) − Ts. Then y′ = T′ and k(T − Ts) = ky. The equation now looks like dT dt = k(T − Ts) ⇐⇒ dy dt = ky Now we can solve! y′ = ky =⇒ y = Cekt =⇒ T − Ts = Cekt =⇒ T = Cekt + Ts V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
  • 62. . . . . . . General Solution to NLC problems To solve this, change the variable y(t) = T(t) − Ts. Then y′ = T′ and k(T − Ts) = ky. The equation now looks like dT dt = k(T − Ts) ⇐⇒ dy dt = ky Now we can solve! y′ = ky =⇒ y = Cekt =⇒ T − Ts = Cekt =⇒ T = Cekt + Ts Plugging in t = 0, we see C = y0 = T0 − Ts. So Theorem The solution to the equation T′ (t) = k(T(t) − Ts), T(0) = T0 is T(t) = (T0 − Ts)ekt + Ts V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 28 / 40
  • 63. . . . . . . Computing cooling time with NLC Example A hard-boiled egg at 98 ◦ C is put in a sink of 18 ◦ C water. After 5 minutes, the egg’s temperature is 38 ◦ C. Assuming the water has not warmed appreciably, how much longer will it take the egg to reach 20 ◦ C? V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 29 / 40
  • 64. . . . . . . Computing cooling time with NLC Example A hard-boiled egg at 98 ◦ C is put in a sink of 18 ◦ C water. After 5 minutes, the egg’s temperature is 38 ◦ C. Assuming the water has not warmed appreciably, how much longer will it take the egg to reach 20 ◦ C? Solution We know that the temperature function takes the form T(t) = (T0 − Ts)ekt + Ts = 80ekt + 18 To find k, plug in t = 5: 38 = T(5) = 80e5k + 18 and solve for k. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 29 / 40
  • 65. . . . . . . Finding k Solution (Continued) 38 = T(5) = 80e5k + 18 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
  • 66. . . . . . . Finding k Solution (Continued) 38 = T(5) = 80e5k + 18 20 = 80e5k V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
  • 67. . . . . . . Finding k Solution (Continued) 38 = T(5) = 80e5k + 18 20 = 80e5k 1 4 = e5k V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
  • 68. . . . . . . Finding k Solution (Continued) 38 = T(5) = 80e5k + 18 20 = 80e5k 1 4 = e5k ln ( 1 4 ) = 5k V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
  • 69. . . . . . . Finding k Solution (Continued) 38 = T(5) = 80e5k + 18 20 = 80e5k 1 4 = e5k ln ( 1 4 ) = 5k =⇒ k = − 1 5 ln 4. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
  • 70. . . . . . . Finding k Solution (Continued) 38 = T(5) = 80e5k + 18 20 = 80e5k 1 4 = e5k ln ( 1 4 ) = 5k =⇒ k = − 1 5 ln 4. Now we need to solve for t: 20 = T(t) = 80e− t 5 ln 4 + 18 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 30 / 40
  • 71. . . . . . . Finding t Solution (Continued) 20 = 80e− t 5 ln 4 + 18 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
  • 72. . . . . . . Finding t Solution (Continued) 20 = 80e− t 5 ln 4 + 18 2 = 80e− t 5 ln 4 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
  • 73. . . . . . . Finding t Solution (Continued) 20 = 80e− t 5 ln 4 + 18 2 = 80e− t 5 ln 4 1 40 = e− t 5 ln 4 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
  • 74. . . . . . . Finding t Solution (Continued) 20 = 80e− t 5 ln 4 + 18 2 = 80e− t 5 ln 4 1 40 = e− t 5 ln 4 − ln 40 = − t 5 ln 4 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
  • 75. . . . . . . Finding t Solution (Continued) 20 = 80e− t 5 ln 4 + 18 2 = 80e− t 5 ln 4 1 40 = e− t 5 ln 4 − ln 40 = − t 5 ln 4 =⇒ t = ln 40 1 5 ln 4 = 5 ln 40 ln 4 ≈ 13 min V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 31 / 40
  • 76. . . . . . . Computing time of death with NLC Example A murder victim is discovered at midnight and the temperature of the body is recorded as 31 ◦ C. One hour later, the temperature of the body is 29 ◦ C. Assume that the surrounding air temperature remains constant at 21 ◦ C. Calculate the victim’s time of death. (The “normal” temperature of a living human being is approximately 37 ◦ C.) V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 32 / 40
  • 77. . . . . . . Solution Let time 0 be midnight. We know T0 = 31, Ts = 21, and T(1) = 29. We want to know the t for which T(t) = 37. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 33 / 40
  • 78. . . . . . . Solution Let time 0 be midnight. We know T0 = 31, Ts = 21, and T(1) = 29. We want to know the t for which T(t) = 37. To find k: 29 = 10ek·1 + 21 =⇒ k = ln 0.8 V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 33 / 40
  • 79. . . . . . . Solution Let time 0 be midnight. We know T0 = 31, Ts = 21, and T(1) = 29. We want to know the t for which T(t) = 37. To find k: 29 = 10ek·1 + 21 =⇒ k = ln 0.8 To find t: 37 = 10et·ln(0.8) + 21 1.6 = et·ln(0.8) t = ln(1.6) ln(0.8) ≈ −2.10 hr So the time of death was just before 10:00pm. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 33 / 40
  • 80. . . . . . . Outline Recall The differential equation y′ = ky Modeling simple population growth Modeling radioactive decay Carbon-14 Dating Newton’s Law of Cooling Continuously Compounded Interest V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 34 / 40
  • 81. . . . . . . Interest If an account has an compound interest rate of r per year compounded n times, then an initial deposit of A0 dollars becomes A0 ( 1 + r n )nt after t years. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 35 / 40
  • 82. . . . . . . Interest If an account has an compound interest rate of r per year compounded n times, then an initial deposit of A0 dollars becomes A0 ( 1 + r n )nt after t years. For different amounts of compounding, this will change. As n → ∞, we get continously compounded interest A(t) = lim n→∞ A0 ( 1 + r n )nt = A0ert . V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 35 / 40
  • 83. . . . . . . Interest If an account has an compound interest rate of r per year compounded n times, then an initial deposit of A0 dollars becomes A0 ( 1 + r n )nt after t years. For different amounts of compounding, this will change. As n → ∞, we get continously compounded interest A(t) = lim n→∞ A0 ( 1 + r n )nt = A0ert . Thus dollars are like bacteria. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 35 / 40
  • 84. . . . . . . Continuous vs. Discrete Compounding of interest Example Consider two bank accounts: one with 10% annual interested compounded quarterly and one with annual interest rate r compunded continuously. If they produce the same balance after every year, what is r? V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 36 / 40
  • 85. . . . . . . Continuous vs. Discrete Compounding of interest Example Consider two bank accounts: one with 10% annual interested compounded quarterly and one with annual interest rate r compunded continuously. If they produce the same balance after every year, what is r? Solution The balance for the 10% compounded quarterly account after t years is A1(t) = A0(1.025)4t = P((1.025)4 )t The balance for the interest rate r compounded continuously account after t years is A2(t) = A0ert V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 36 / 40
  • 86. . . . . . . Solving Solution (Continued) A1(t) = A0((1.025)4 )t A2(t) = A0(er )t For those to be the same, er = (1.025)4 , so r = ln((1.025)4 ) = 4 ln 1.025 ≈ 0.0988 So 10% annual interest compounded quarterly is basically equivalent to 9.88% compounded continuously. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 37 / 40
  • 87. . . . . . . Computing doubling time with exponential growth Example How long does it take an initial deposit of $100, compounded continuously, to double? V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 38 / 40
  • 88. . . . . . . Computing doubling time with exponential growth Example How long does it take an initial deposit of $100, compounded continuously, to double? Solution We need t such that A(t) = 200. In other words 200 = 100ert =⇒ 2 = ert =⇒ ln 2 = rt =⇒ t = ln 2 r . For instance, if r = 6% = 0.06, we have t = ln 2 0.06 ≈ 0.69 0.06 = 69 6 = 11.5 years. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 38 / 40
  • 89. . . . . . . I-banking interview tip of the day The fraction ln 2 r can also be approximated as either 70 or 72 divided by the percentage rate (as a number between 0 and 100, not a fraction between 0 and 1.) This is sometimes called the rule of 70 or rule of 72. 72 has lots of factors so it’s used more often. V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 39 / 40
  • 90. . . . . . . Summary When something grows or decays at a constant relative rate, the growth or decay is exponential. Equations with unknowns in an exponent can be solved with logarithms. Your friend list is like culture of bacteria (no offense). V63.0121.021, Calculus I (NYU) Section 3.4 Exponential Growth and Decay October 28, 2010 40 / 40