lecture 7: velocity, rate of change, and the...
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Velocity Rate of Change The Derivative
Lecture 7: Velocity, Rate of Change, and the Derivative
VelocityRepresenting MotionAverage VelocityInstantaneous VelocityExample 25 – Computing Velocities from a GraphEstimating Slope by Averaging – Straddling
Rate of ChangeAverage Rate of ChangeInstantaneous Rate of ChangeExample 26 – Rate of Change of Area
The DerivativeThe Derivative at a PointMeanings of the Derivative at a PointExamples of DerivativesExample 27 – Calculating a Derivative at a Point
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 1/30
Velocity Rate of Change The Derivative
Representing Motion
Representing Motion
Motion Along a Line
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 2/30
Velocity Rate of Change The Derivative
Representing Motion
Representing Motion
Motion Along a Line
For an object moving along a straightline the position along the line relativeto some origin is given by s = f (t),
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 2/30
Velocity Rate of Change The Derivative
Representing Motion
Representing Motion
Motion Along a Line
For an object moving along a straightline the position along the line relativeto some origin is given by s = f (t),where s is a real number representingthe distance, positive to the right andnegative to the left, from the origin.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 2/30
Velocity Rate of Change The Derivative
Representing Motion
Representing Motion
Motion Along a Line
For an object moving along a straightline the position along the line relativeto some origin is given by s = f (t),where s is a real number representingthe distance, positive to the right andnegative to the left, from the origin.The function f is the position functionof the object.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 2/30
Velocity Rate of Change The Derivative
Representing Motion
Representing Motion
Motion Along a Line
For an object moving along a straightline the position along the line relativeto some origin is given by s = f (t),where s is a real number representingthe distance, positive to the right andnegative to the left, from the origin.The function f is the position functionof the object. The motion of the objectcan be represented in a diagram likethis.
0
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 2/30
Velocity Rate of Change The Derivative
Representing Motion
Representing Motion
Motion Along a Line
For an object moving along a straightline the position along the line relativeto some origin is given by s = f (t),where s is a real number representingthe distance, positive to the right andnegative to the left, from the origin.The function f is the position functionof the object. The motion of the objectcan be represented in a diagram likethis.
0
t=0
t=16t=2
t
s
s= f (t)
2 16
We get more information about the motion of the object by graphing fas a function of t, like this.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 2/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity
The velocity of a moving object is the displacement or change inposition per unit time.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 3/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity
The velocity of a moving object is the displacement or change inposition per unit time. Velocity can be positive, negative, or zero(even if the body is moving).
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 3/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity
The velocity of a moving object is the displacement or change inposition per unit time. Velocity can be positive, negative, or zero(even if the body is moving).The speed of the object is the total distance traveled per unit time,which can be different than the velocity and is always positive.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 3/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity
The velocity of a moving object is the displacement or change inposition per unit time. Velocity can be positive, negative, or zero(even if the body is moving).The speed of the object is the total distance traveled per unit time,which can be different than the velocity and is always positive.
Average Velocity
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 3/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity
The velocity of a moving object is the displacement or change inposition per unit time. Velocity can be positive, negative, or zero(even if the body is moving).The speed of the object is the total distance traveled per unit time,which can be different than the velocity and is always positive.
Average Velocity
The average velocity of the object whose position is given by s = f (t)over the time interval between t = t1 and t = t2 is
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 3/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity
The velocity of a moving object is the displacement or change inposition per unit time. Velocity can be positive, negative, or zero(even if the body is moving).The speed of the object is the total distance traveled per unit time,which can be different than the velocity and is always positive.
Average Velocity
The average velocity of the object whose position is given by s = f (t)over the time interval between t = t1 and t = t2 is
vave =f (t2) − f (t1)
t2 − t1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 3/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity
The velocity of a moving object is the displacement or change inposition per unit time. Velocity can be positive, negative, or zero(even if the body is moving).The speed of the object is the total distance traveled per unit time,which can be different than the velocity and is always positive.
Average Velocity
The average velocity of the object whose position is given by s = f (t)over the time interval between t = t1 and t = t2 is
vave =f (t2) − f (t1)
t2 − t1=
f (t1) − f (t2)
t1 − t2
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 3/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity
The velocity of a moving object is the displacement or change inposition per unit time. Velocity can be positive, negative, or zero(even if the body is moving).The speed of the object is the total distance traveled per unit time,which can be different than the velocity and is always positive.
Average Velocity
The average velocity of the object whose position is given by s = f (t)over the time interval between t = t1 and t = t2 is
vave =f (t2) − f (t1)
t2 − t1=
f (t1) − f (t2)
t1 − t2
The value (and sign) of the average velocity does not depend onwhich order we take for the times.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 3/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity as a Slope
The formula for the average velocityshould look familiar. It just represents theslope of the line joining the two points(t1, f (t1)) and (t2, f (t2)) on the graph ofthe position function.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 4/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity as a Slope
The formula for the average velocityshould look familiar. It just represents theslope of the line joining the two points(t1, f (t1)) and (t2, f (t2)) on the graph ofthe position function. With t2 after t1 itlooks like this.
t
s
t1 t2
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 4/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity as a Slope
The formula for the average velocityshould look familiar. It just represents theslope of the line joining the two points(t1, f (t1)) and (t2, f (t2)) on the graph ofthe position function. With t2 after t1 itlooks like this. With time t2 before t1, likethis.
t
s
t1t2
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 4/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity as a Slope
To make the formula for average velocitylook more familiar let t1 = a andt2 = a + h. If h > 0, then t2 is later than t1,and if h < 0, then t2 is earlier than t1.
t
s
t1 t2
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 5/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity as a Slope
To make the formula for average velocitylook more familiar let t1 = a andt2 = a + h. If h > 0, then t2 is later than t1,and if h < 0, then t2 is earlier than t1. Likethis.
t
s
a a+h
h
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 5/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity as a Slope
To make the formula for average velocitylook more familiar let t1 = a andt2 = a + h. If h > 0, then t2 is later than t1,and if h < 0, then t2 is earlier than t1. Likethis.
Alternate Formula for Average Velocity
The formula for the average velocity canbe written
vave =
t
s
a a+h
h
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 5/30
Velocity Rate of Change The Derivative
Average Velocity
Average Velocity as a Slope
To make the formula for average velocitylook more familiar let t1 = a andt2 = a + h. If h > 0, then t2 is later than t1,and if h < 0, then t2 is earlier than t1. Likethis.
Alternate Formula for Average Velocity
The formula for the average velocity canbe written
vave =f (a + h) − f (a)
h
t
s
a a+h
h
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 5/30
Velocity Rate of Change The Derivative
Instantaneous Velocity
Instantaneous Velocity
The instantaneous velocity of a movingobject can be found by taking the averagevelocity over shorter and shorter timeintervals. This means we take t2 closer tot1, from either side of t1.
t
s
a a+h
h
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 6/30
Velocity Rate of Change The Derivative
Instantaneous Velocity
Instantaneous Velocity
The instantaneous velocity of a movingobject can be found by taking the averagevelocity over shorter and shorter timeintervals. This means we take t2 closer tot1, from either side of t1. Equivalently, thismeans taking h closer and closer to zero,from above or below.
t
s
a a+h
h
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 6/30
Velocity Rate of Change The Derivative
Instantaneous Velocity
Instantaneous Velocity
Instantaneous Velocity
The instantaneous velocity of an objectmoving along a straight line withposition function s = f (t) at time t = a is
t
s
a a+h
h
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 7/30
Velocity Rate of Change The Derivative
Instantaneous Velocity
Instantaneous Velocity
Instantaneous Velocity
The instantaneous velocity of an objectmoving along a straight line withposition function s = f (t) at time t = a is
v(a)
t
s
a a+h
h
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 7/30
Velocity Rate of Change The Derivative
Instantaneous Velocity
Instantaneous Velocity
Instantaneous Velocity
The instantaneous velocity of an objectmoving along a straight line withposition function s = f (t) at time t = a is
v(a) = limh→0
f (a + h) − f (a)
h
t
s
a a+h
h
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 7/30
Velocity Rate of Change The Derivative
Instantaneous Velocity
Instantaneous Velocity
Instantaneous Velocity
The instantaneous velocity of an objectmoving along a straight line withposition function s = f (t) at time t = a is
v(a) = limh→0
f (a + h) − f (a)
h
The instantaneous velocity is the slope ofthe tangent line to the graph of theposition function at t = a, as shown in thegraph.
t
s
a
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 7/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Example 25 – Computing Velocities from a Graph
The graph shows the position functions = f (t) of an object moving along astraight line with the distance, s, from theorigin given in metres and the time, t, inseconds.
(a) Compute the average velocity ofthe object over time intervals:
t = 10 to t = 14t = 6 to t = 10
2
4
6
8
10
4 8 12 t (s)
s (m)
s= f (t)
(c) Estimate the instantaneous velocity of the object at t = 10 byaveraging the two average velocities in part (a).
(d) Estimate the instantaneous velocity by computing the slope ofthe tangent to the graph of the position function at t = 10.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 8/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2, f (14) = 10
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2, f (14) = 10
For the interval from t = 10 to t = 14 take a = 10 and h = 4, so that
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2, f (14) = 10
For the interval from t = 10 to t = 14 take a = 10 and h = 4, so that
vave =f (14) − f (10)
4= 2
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2, f (14) = 10
For the interval from t = 10 to t = 14 take a = 10 and h = 4, so that
vave =f (14) − f (10)
4= 2
For the interval from t = 6 to t = 10 take a = 10 and h = −4, so that
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2, f (14) = 10
For the interval from t = 10 to t = 14 take a = 10 and h = 4, so that
vave =f (14) − f (10)
4= 2
For the interval from t = 6 to t = 10 take a = 10 and h = −4, so that
vave =f (6) − f (10)
−4=
3
4
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2, f (14) = 10
For the interval from t = 10 to t = 14 take a = 10 and h = 4, so that
vave =f (14) − f (10)
4= 2
For the interval from t = 6 to t = 10 take a = 10 and h = −4, so that
vave =f (6) − f (10)
−4=
3
4
Then an estimate of the instantaneous velocity at t = 10 is theaverage of these two values
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2, f (14) = 10
For the interval from t = 10 to t = 14 take a = 10 and h = 4, so that
vave =f (14) − f (10)
4= 2
For the interval from t = 6 to t = 10 take a = 10 and h = −4, so that
vave =f (6) − f (10)
−4=
3
4
Then an estimate of the instantaneous velocity at t = 10 is theaverage of these two values
v(10)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(a) & (b)
Reading off the graph we have
f (6) = − 1, f (10) = 2, f (14) = 10
For the interval from t = 10 to t = 14 take a = 10 and h = 4, so that
vave =f (14) − f (10)
4= 2
For the interval from t = 6 to t = 10 take a = 10 and h = −4, so that
vave =f (6) − f (10)
−4=
3
4
Then an estimate of the instantaneous velocity at t = 10 is theaverage of these two values
v(10) ≈1
2
(
2 +3
4
)
=11
8= 1.375 m/s
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 9/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(c)
The tangent to the graph of the positionfunction at t = 10 is shown.
2
4
6
8
10
4 8 12 t (s)
s (m)
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 10/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(c)
The tangent to the graph of the positionfunction at t = 10 is shown.
Reading from the graph the tangent linegoes through the points (6.6,−2.0) and(14.0, 6.9).
2
4
6
8
10
4 8 12 t (s)
s (m)
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 10/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(c)
The tangent to the graph of the positionfunction at t = 10 is shown.
Reading from the graph the tangent linegoes through the points (6.6,−2.0) and(14.0, 6.9). So the slope of the tangent lineis
mT =6.9 − (−2.0)
14.9 − 6.6
2
4
6
8
10
4 8 12 t (s)
s (m)
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 10/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(c)
The tangent to the graph of the positionfunction at t = 10 is shown.
Reading from the graph the tangent linegoes through the points (6.6,−2.0) and(14.0, 6.9). So the slope of the tangent lineis
mT =6.9 − (−2.0)
14.9 − 6.6= 1.20 m/s
2
4
6
8
10
4 8 12 t (s)
s (m)
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 10/30
Velocity Rate of Change The Derivative
Example 25 – Computing Velocities from a Graph
Solution: Example 25(c)
The tangent to the graph of the positionfunction at t = 10 is shown.
Reading from the graph the tangent linegoes through the points (6.6,−2.0) and(14.0, 6.9). So the slope of the tangent lineis
mT =6.9 − (−2.0)
14.9 − 6.6= 1.20 m/s
Since the slope of the tangent at t = 10equals the instantaneous velocity att = 10, the instantaneous velocity att = 10 is estimated to be 1.20 m/s.
2
4
6
8
10
4 8 12 t (s)
s (m)
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 10/30
Velocity Rate of Change The Derivative
Estimating Slope by Averaging – Straddling
Estimating Slope by Averaging – Straddling
In Example 25(b) we estimated the slopeof the tangent line, and hence theinstantaneous velocity, by averaging theslopes of two secant lines. The calculationis
v(10) ≈1
2
(
f (14) − f (10)
4+
f (6) − f (10)
−4
) 2
4
6
8
10
4 8 12 t (s)
s (m)
10
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 11/30
Velocity Rate of Change The Derivative
Estimating Slope by Averaging – Straddling
Estimating Slope by Averaging – Straddling
In Example 25(b) we estimated the slopeof the tangent line, and hence theinstantaneous velocity, by averaging theslopes of two secant lines. The calculationis
v(10) ≈1
2
(
f (14) − f (10)
4+
f (6) − f (10)
−4
)
=f (14) − f (6)
8
2
4
6
8
10
4 8 12 t (s)
s (m)
10
s= f (t)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 11/30
Velocity Rate of Change The Derivative
Estimating Slope by Averaging – Straddling
Estimating Slope by Averaging – Straddling
In Example 25(b) we estimated the slopeof the tangent line, and hence theinstantaneous velocity, by averaging theslopes of two secant lines. The calculationis
v(10) ≈1
2
(
f (14) − f (10)
4+
f (6) − f (10)
−4
)
=f (14) − f (6)
8
2
4
6
8
10
4 8 12 t (s)
s (m)
10
s= f (t)
This means we can estimate the slope of the tangent line at a point bycomputing the slope of a secant line joining two points on either sideof the point, at an equal distance on either side. See the diagram.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 11/30
Velocity Rate of Change The Derivative
Estimating Slope by Averaging – Straddling
Estimating Slope by Averaging – Straddling
In Example 25(b) we estimated the slopeof the tangent line, and hence theinstantaneous velocity, by averaging theslopes of two secant lines. The calculationis
v(10) ≈1
2
(
f (14) − f (10)
4+
f (6) − f (10)
−4
)
=f (14) − f (6)
8
2
4
6
8
10
4 8 12 t (s)
s (m)
10
s= f (t)
This means we can estimate the slope of the tangent line at a point bycomputing the slope of a secant line joining two points on either sideof the point, at an equal distance on either side. See the diagram. This isstraddling. The straddling secant line has a slope at least as close to the slopeof the tangent as either of the one-sided secant lines.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 11/30
Velocity Rate of Change The Derivative
Estimating Slope by Averaging – Straddling
Estimating Slope by Averaging – Straddling
In Example 25(b) we estimated the slopeof the tangent line, and hence theinstantaneous velocity, by averaging theslopes of two secant lines. The calculationis
v(10) ≈1
2
(
f (14) − f (10)
4+
f (6) − f (10)
−4
)
=f (14) − f (6)
8
2
4
6
8
10
4 8 12 t (s)
s (m)
10
s= f (t)
This means we can estimate the slope of the tangent line at a point bycomputing the slope of a secant line joining two points on either sideof the point, at an equal distance on either side. See the diagram. This isstraddling. The straddling secant line has a slope at least as close to the slopeof the tangent as either of the one-sided secant lines.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 11/30
Velocity Rate of Change The Derivative
Average Rate of Change
Increments
If quantity y is a function of quantity x, y = f (x),
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 12/30
Velocity Rate of Change The Derivative
Average Rate of Change
Increments
If quantity y is a function of quantity x, y = f (x), and, if x changesfrom x1 to x2, the increment in x is
∆x = x2 − x1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 12/30
Velocity Rate of Change The Derivative
Average Rate of Change
Increments
If quantity y is a function of quantity x, y = f (x), and, if x changesfrom x1 to x2, the increment in x is
∆x = x2 − x1
and y changes from f (x1) to f (x2) for an increment of
∆y = f (x2) − f (x1)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 12/30
Velocity Rate of Change The Derivative
Average Rate of Change
Average Rate of Change
Average Rate of Change
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 13/30
Velocity Rate of Change The Derivative
Average Rate of Change
Average Rate of Change
Average Rate of Change
The average rate of change of y with respect to x when x changesfrom x1 to x2 is
average rate of change
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 13/30
Velocity Rate of Change The Derivative
Average Rate of Change
Average Rate of Change
Average Rate of Change
The average rate of change of y with respect to x when x changesfrom x1 to x2 is
average rate of change =f (x2) − f (x1)
x2 − x1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 13/30
Velocity Rate of Change The Derivative
Average Rate of Change
Average Rate of Change
Average Rate of Change
The average rate of change of y with respect to x when x changesfrom x1 to x2 is
average rate of change =f (x2) − f (x1)
x2 − x1=
∆y
∆x
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 13/30
Velocity Rate of Change The Derivative
Average Rate of Change
Average Rate of Change
Average Rate of Change
The average rate of change of y with respect to x when x changesfrom x1 to x2 is
average rate of change =f (x2) − f (x1)
x2 − x1=
∆y
∆x
This rate of change can also be described as the change in y per unitchange in x.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 13/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
As x2 gets closer and closer to x1, the average rate of changeapproaches the instantaneous rate of change of y with respect to x atx = x1.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 14/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
As x2 gets closer and closer to x1, the average rate of changeapproaches the instantaneous rate of change of y with respect to x atx = x1. As x2 → x1, the increment ∆x → 0.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 14/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
As x2 gets closer and closer to x1, the average rate of changeapproaches the instantaneous rate of change of y with respect to x atx = x1. As x2 → x1, the increment ∆x → 0.
Instantaneous Rate of Change at x1
instantaneous rate of change = limx2→x1
f (x2) − f (x1)
x2 − x1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 14/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
As x2 gets closer and closer to x1, the average rate of changeapproaches the instantaneous rate of change of y with respect to x atx = x1. As x2 → x1, the increment ∆x → 0.
Instantaneous Rate of Change at x1
instantaneous rate of change = limx2→x1
f (x2) − f (x1)
x2 − x1= lim
∆x→0
∆y
∆x
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 14/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
Letting x1 = a and ∆x = h, we have
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 15/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
Letting x1 = a and ∆x = h, we have x2 = x1 + ∆x
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 15/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
Letting x1 = a and ∆x = h, we have x2 = x1 + ∆x = a + h.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 15/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
Letting x1 = a and ∆x = h, we have x2 = x1 + ∆x = a + h.
Instantaneous Rate of Change at a
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 15/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
Letting x1 = a and ∆x = h, we have x2 = x1 + ∆x = a + h.
Instantaneous Rate of Change at a
The definition of instantaneous rate of change can be written
instantaneous rate of change
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 15/30
Velocity Rate of Change The Derivative
Instantaneous Rate of Change
Instantaneous Rate of Change
Letting x1 = a and ∆x = h, we have x2 = x1 + ∆x = a + h.
Instantaneous Rate of Change at a
The definition of instantaneous rate of change can be written
instantaneous rate of change = limh→0
f (a + h) − f (a)
h
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 15/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Example 26 – Rate of Change of Area
The area A of a square with side length s is A = f (s) = s2.
(a) Determine the average rate of change of the area of a squarewhen the side length changes from
s = 5 m to s = 6 ms = 5 m to s = 5.5 ms = 5 m to s = 5.1 m
Give the units of the rate of change.
(b) Determine the instantaneous rate of change of the area of thesquare with respect to its side length when the side length iss = 5 m.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 16/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(a)
The average rates of change are
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 17/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(a)
The average rates of change are
f (6) − f (5)
6 − 5=
36 − 25
1= 11
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 17/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(a)
The average rates of change are
f (6) − f (5)
6 − 5=
36 − 25
1= 11
f (5.5) − f (5)
5.5 − 5=
30.25 − 25
0.5= 10.5
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 17/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(a)
The average rates of change are
f (6) − f (5)
6 − 5=
36 − 25
1= 11
f (5.5) − f (5)
5.5 − 5=
30.25 − 25
0.5= 10.5
f (5.1) − f (5)
5.1 − 5=
26.01 − 25
0.1= 10.1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 17/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(a)
The average rates of change are
f (6) − f (5)
6 − 5=
36 − 25
1= 11
f (5.5) − f (5)
5.5 − 5=
30.25 − 25
0.5= 10.5
f (5.1) − f (5)
5.1 − 5=
26.01 − 25
0.1= 10.1
In each case the units of the rate of change are m2/m or just metres.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 17/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(b)
The instantaneous rate of change is given by
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 18/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(b)
The instantaneous rate of change is given by
lim∆s→0
f (5 + ∆s) − f (5)
∆s
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 18/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(b)
The instantaneous rate of change is given by
lim∆s→0
f (5 + ∆s) − f (5)
∆s= lim
∆s→0
(5 + ∆s)2− 25
∆s
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 18/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(b)
The instantaneous rate of change is given by
lim∆s→0
f (5 + ∆s) − f (5)
∆s= lim
∆s→0
(5 + ∆s)2− 25
∆s
= lim∆s→0
25 + 10∆s + ∆s2− 25
∆s
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 18/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(b)
The instantaneous rate of change is given by
lim∆s→0
f (5 + ∆s) − f (5)
∆s= lim
∆s→0
(5 + ∆s)2− 25
∆s
= lim∆s→0
25 + 10∆s + ∆s2− 25
∆s
= lim∆s→0
(10 + ∆s)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 18/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(b)
The instantaneous rate of change is given by
lim∆s→0
f (5 + ∆s) − f (5)
∆s= lim
∆s→0
(5 + ∆s)2− 25
∆s
= lim∆s→0
25 + 10∆s + ∆s2− 25
∆s
= lim∆s→0
(10 + ∆s) = 10
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 18/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26(b)
The instantaneous rate of change is given by
lim∆s→0
f (5 + ∆s) − f (5)
∆s= lim
∆s→0
(5 + ∆s)2− 25
∆s
= lim∆s→0
25 + 10∆s + ∆s2− 25
∆s
= lim∆s→0
(10 + ∆s) = 10
This agrees with the trend in the values found in part (a).
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 18/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area.
s = 5
∆s = 1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area. This area ismade up of three parts, two rectangles anda small square. The combined area is2 × 5 × 1 + 1 × 1 = 11.
s = 5
∆s = 1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area. This area ismade up of three parts, two rectangles anda small square. The combined area is2 × 5 × 1 + 1 × 1 = 11. And thecorresponding average rate of change of thearea is 2 × 5 + 1 = 11.
s = 5
∆s = 1
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area. This area ismade up of three parts, two rectangles anda small square. The combined area is2 × 5 × 1 + 1 × 1 = 11. And thecorresponding average rate of change of thearea is 2 × 5 + 1 = 11.
s = 5
∆s = 1
When the side length changes from s = 5 m to s = 5.5 m the diagramlooks like this.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area. This area ismade up of three parts, two rectangles anda small square. The combined area is2 × 5 × 1 + 1 × 1 = 11. And thecorresponding average rate of change of thearea is 2 × 5 + 1 = 11.
s = 5
∆s = 0.5
When the side length changes from s = 5 m to s = 5.5 m the diagramlooks like this. The change in area is 2 × 5 × 0.5 + 0.5 × 0.5 = 5.25,
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area. This area ismade up of three parts, two rectangles anda small square. The combined area is2 × 5 × 1 + 1 × 1 = 11. And thecorresponding average rate of change of thearea is 2 × 5 + 1 = 11.
s = 5
∆s = 0.5
When the side length changes from s = 5 m to s = 5.5 m the diagramlooks like this. The change in area is 2 × 5 × 0.5 + 0.5 × 0.5 = 5.25,and the average rate of change is 2 × 5 + 0.5 = 10.5.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area. This area ismade up of three parts, two rectangles anda small square. The combined area is2 × 5 × 1 + 1 × 1 = 11. And thecorresponding average rate of change of thearea is 2 × 5 + 1 = 11.
s = 5
∆s = 0.5
When the side length changes from s = 5 m to s = 5.5 m the diagramlooks like this. The change in area is 2 × 5 × 0.5 + 0.5 × 0.5 = 5.25,and the average rate of change is 2 × 5 + 0.5 = 10.5.
When the side length changes from s = 5 m to s = 5.1 m the diagramlooks like this.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area. This area ismade up of three parts, two rectangles anda small square. The combined area is2 × 5 × 1 + 1 × 1 = 11. And thecorresponding average rate of change of thearea is 2 × 5 + 1 = 11.
When the side length changes from s = 5 m to s = 5.5 m the diagramlooks like this. The change in area is 2 × 5 × 0.5 + 0.5 × 0.5 = 5.25,and the average rate of change is 2 × 5 + 0.5 = 10.5.
When the side length changes from s = 5 m to s = 5.1 m the diagramlooks like this. The change in area is 2 × 5 × 0.1 + 0.1 × 0.1 = 1.01,
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment
Consider the change in the area of thesquare when the side length increases froms = 5 m to s = 6 m. This is shown in thediagram, where the the shaded portionsrepresent the change in area. This area ismade up of three parts, two rectangles anda small square. The combined area is2 × 5 × 1 + 1 × 1 = 11. And thecorresponding average rate of change of thearea is 2 × 5 + 1 = 11.
When the side length changes from s = 5 m to s = 5.5 m the diagramlooks like this. The change in area is 2 × 5 × 0.5 + 0.5 × 0.5 = 5.25,and the average rate of change is 2 × 5 + 0.5 = 10.5.
When the side length changes from s = 5 m to s = 5.1 m the diagramlooks like this. The change in area is 2 × 5 × 0.1 + 0.1 × 0.1 = 1.01,and the average rate of change is 2 × 5 + 0.1 = 10.1.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 19/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
In general, the average rate of change of the area of the square whenthe side length changes from s = 5 to s = 5 + ∆s is
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 20/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
In general, the average rate of change of the area of the square whenthe side length changes from s = 5 to s = 5 + ∆s is
average rate of change of area = 2 × 5 + ∆s
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 20/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
In general, the average rate of change of the area of the square whenthe side length changes from s = 5 to s = 5 + ∆s is
average rate of change of area = 2 × 5 + ∆s
Of course, as ∆s → 0, this average rate of change approaches 2 × 5 m,the instantaneous rate of change of the area with respect to the sidelength. As the change in the side length gets smaller, the contributionof the small square to the rate of change in the area gets smaller,eventually becoming negligible.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 20/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
In general, the average rate of change of the area of the square whenthe side length changes from s = 5 to s = 5 + ∆s is
average rate of change of area = 2 × 5 + ∆s
Of course, as ∆s → 0, this average rate of change approaches 2 × 5 m,the instantaneous rate of change of the area with respect to the sidelength. As the change in the side length gets smaller, the contributionof the small square to the rate of change in the area gets smaller,eventually becoming negligible.
This value is twice the side length of the square, or, alternatively, onehalf of the perimeter of the square. So we can say
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 20/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
In general, the average rate of change of the area of the square whenthe side length changes from s = 5 to s = 5 + ∆s is
average rate of change of area = 2 × 5 + ∆s
Of course, as ∆s → 0, this average rate of change approaches 2 × 5 m,the instantaneous rate of change of the area with respect to the sidelength. As the change in the side length gets smaller, the contributionof the small square to the rate of change in the area gets smaller,eventually becoming negligible.
This value is twice the side length of the square, or, alternatively, onehalf of the perimeter of the square. So we can say
instantaneous rate of change ofarea of square with respect to sidelength
=1
2perimeter of the square
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 20/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
This is true for a square of side length a, since
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 21/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
This is true for a square of side length a, since
lim∆s→0
f (a + ∆s) − f (a)
∆s
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 21/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
This is true for a square of side length a, since
lim∆s→0
f (a + ∆s) − f (a)
∆s= lim
∆s→0
(a + ∆s)2− a2
∆s
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 21/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
This is true for a square of side length a, since
lim∆s→0
f (a + ∆s) − f (a)
∆s= lim
∆s→0
(a + ∆s)2− a2
∆s
= lim∆s→0
a2 + 2a∆s + ∆s2− a2
∆s
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 21/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
This is true for a square of side length a, since
lim∆s→0
f (a + ∆s) − f (a)
∆s= lim
∆s→0
(a + ∆s)2− a2
∆s
= lim∆s→0
a2 + 2a∆s + ∆s2− a2
∆s
= lim∆s→0
(2a + ∆s)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 21/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
This is true for a square of side length a, since
lim∆s→0
f (a + ∆s) − f (a)
∆s= lim
∆s→0
(a + ∆s)2− a2
∆s
= lim∆s→0
a2 + 2a∆s + ∆s2− a2
∆s
= lim∆s→0
(2a + ∆s)
= 2a
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 21/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
This is true for a square of side length a, since
lim∆s→0
f (a + ∆s) − f (a)
∆s= lim
∆s→0
(a + ∆s)2− a2
∆s
= lim∆s→0
a2 + 2a∆s + ∆s2− a2
∆s
= lim∆s→0
(2a + ∆s)
= 2a =1
2perimeter of square
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 21/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Solution: Example 26 Comment continued
This is true for a square of side length a, since
lim∆s→0
f (a + ∆s) − f (a)
∆s= lim
∆s→0
(a + ∆s)2− a2
∆s
= lim∆s→0
a2 + 2a∆s + ∆s2− a2
∆s
= lim∆s→0
(2a + ∆s)
= 2a =1
2perimeter of square
To pursue this idea further, express the area of a square as a functionof the distance x of each side of the square from its centre. Show thatthe rate of change of the area of the square with respect to x equalsthe perimeter of the square, and draw a diagram to understand howthis result comes about.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 21/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Other Rates of Change
Slope and Velocity as Rates of Change
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 22/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Other Rates of Change
Slope and Velocity as Rates of Change
The slope of a line is the rate of change of the y-coordinate ofpoints on the line with respect to the x-coordinate.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 22/30
Velocity Rate of Change The Derivative
Example 26 – Rate of Change of Area
Other Rates of Change
Slope and Velocity as Rates of Change
The slope of a line is the rate of change of the y-coordinate ofpoints on the line with respect to the x-coordinate.
The velocity of a moving object is the rate of change of theposition of the object with respect to time.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 22/30
Velocity Rate of Change The Derivative
The Derivative at a Point
The Derivative at a Point
Derivative at a Point
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 23/30
Velocity Rate of Change The Derivative
The Derivative at a Point
The Derivative at a Point
Derivative at a Point
For a function f defined at x = a, the derivative of f at a is
f ′(a) 1
2
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 23/30
Velocity Rate of Change The Derivative
The Derivative at a Point
The Derivative at a Point
Derivative at a Point
For a function f defined at x = a, the derivative of f at a is
f ′(a) = limx→a
f (x) − f (a)
x − a1
2
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 23/30
Velocity Rate of Change The Derivative
The Derivative at a Point
The Derivative at a Point
Derivative at a Point
For a function f defined at x = a, the derivative of f at a is
f ′(a) = limx→a
f (x) − f (a)
x − a1
= limh→0
f (a + h) − f (a)
h2
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 23/30
Velocity Rate of Change The Derivative
Meanings of the Derivative at a Point
Meanings of the Derivative at a Point
Meanings of the Derivative at a Point
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 24/30
Velocity Rate of Change The Derivative
Meanings of the Derivative at a Point
Meanings of the Derivative at a Point
Meanings of the Derivative at a Point
There are three interpretations, or applications, of the derivative at apoint
The slope of the tangent line to the graph of f at the point(a, f (a)).This is also called the slope of the linearization of f at a, or justthe slope of the curve y = f (x) at (a, f (a)).
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 24/30
Velocity Rate of Change The Derivative
Meanings of the Derivative at a Point
Meanings of the Derivative at a Point
Meanings of the Derivative at a Point
There are three interpretations, or applications, of the derivative at apoint
The slope of the tangent line to the graph of f at the point(a, f (a)).This is also called the slope of the linearization of f at a, or justthe slope of the curve y = f (x) at (a, f (a)).
The (instantaneous) velocity at time t = a of a moving objectwhose position at time t is given by s = f (t).
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 24/30
Velocity Rate of Change The Derivative
Meanings of the Derivative at a Point
Meanings of the Derivative at a Point
Meanings of the Derivative at a Point
There are three interpretations, or applications, of the derivative at apoint
The slope of the tangent line to the graph of f at the point(a, f (a)).This is also called the slope of the linearization of f at a, or justthe slope of the curve y = f (x) at (a, f (a)).
The (instantaneous) velocity at time t = a of a moving objectwhose position at time t is given by s = f (t).
The (instantaneous) rate of change of the quantity y with respectto the quantity x at x = a, when y = f (x).
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 24/30
Velocity Rate of Change The Derivative
Examples of Derivatives
Examples of Derivatives
We have already computed or estimated derivatives.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 25/30
Velocity Rate of Change The Derivative
Examples of Derivatives
Examples of Derivatives
We have already computed or estimated derivatives.
In Example 22 for the function f (x) = x3 we found that f ′(1) = 3.In this example the derivative gave us the slope, and so theequation of the line tangent to y = x3 at the point (1, 1).
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 25/30
Velocity Rate of Change The Derivative
Examples of Derivatives
Examples of Derivatives
We have already computed or estimated derivatives.
In Example 22 for the function f (x) = x3 we found that f ′(1) = 3.In this example the derivative gave us the slope, and so theequation of the line tangent to y = x3 at the point (1, 1).
In Example 25 we estimated f ′(10) to give the instantaneousvelocity of a moving object whose position is given by s = f (t).The estimate was based on the graph of the function f .
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 25/30
Velocity Rate of Change The Derivative
Examples of Derivatives
Examples of Derivatives
We have already computed or estimated derivatives.
In Example 22 for the function f (x) = x3 we found that f ′(1) = 3.In this example the derivative gave us the slope, and so theequation of the line tangent to y = x3 at the point (1, 1).
In Example 25 we estimated f ′(10) to give the instantaneousvelocity of a moving object whose position is given by s = f (t).The estimate was based on the graph of the function f .
In Example 26 for the function A = f (s) = s2 we found thatf ′(5) = 10, and, more generally, that f ′(a) = 2a. In this examplethe derivative gave us the rate of change of the area A of a squarewith respect to its side length s.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 25/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Example 27 – Calculating a Derivative at a Point
Letf (x) =
x
x − 1
(a) Calculate f ′(3) using Formula 1 .
(b) Calculate f ′(3) using Formula 2 .
(c) Calculate f ′(a) for any number a in the domain of f using
Formula 2 .
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 26/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(a)
First note that f (3) = 3/2. Then applying Formula 1 with
f (x) =x
x − 1and a = 3 gives
f ′(3) =
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 27/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(a)
First note that f (3) = 3/2. Then applying Formula 1 with
f (x) =x
x − 1and a = 3 gives
f ′(3) = limx→3
x
x − 1−
3
2x − 3
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 27/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(a)
First note that f (3) = 3/2. Then applying Formula 1 with
f (x) =x
x − 1and a = 3 gives
f ′(3) = limx→3
x
x − 1−
3
2x − 3
= limx→3
(
2x − 3(x − 1)
2(x − 1)(x − 3)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 27/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(a)
First note that f (3) = 3/2. Then applying Formula 1 with
f (x) =x
x − 1and a = 3 gives
f ′(3) = limx→3
x
x − 1−
3
2x − 3
= limx→3
(
2x − 3(x − 1)
2(x − 1)(x − 3)
)
= limx→3
(
2x − 3x + 3
2(x − 1)(x − 3)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 27/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(a)
First note that f (3) = 3/2. Then applying Formula 1 with
f (x) =x
x − 1and a = 3 gives
f ′(3) = limx→3
x
x − 1−
3
2x − 3
= limx→3
(
2x − 3(x − 1)
2(x − 1)(x − 3)
)
= limx→3
(
2x − 3x + 3
2(x − 1)(x − 3)
)
= limx→3
(
−(x − 3)
2(x − 1)(x − 3)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 27/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(a)
First note that f (3) = 3/2. Then applying Formula 1 with
f (x) =x
x − 1and a = 3 gives
f ′(3) = limx→3
x
x − 1−
3
2x − 3
= limx→3
(
2x − 3(x − 1)
2(x − 1)(x − 3)
)
= limx→3
(
2x − 3x + 3
2(x − 1)(x − 3)
)
= limx→3
(
−(x − 3)
2(x − 1)(x − 3)
)
= limx→3
(
−1
2(x − 1)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 27/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(a)
First note that f (3) = 3/2. Then applying Formula 1 with
f (x) =x
x − 1and a = 3 gives
f ′(3) = limx→3
x
x − 1−
3
2x − 3
= limx→3
(
2x − 3(x − 1)
2(x − 1)(x − 3)
)
= limx→3
(
2x − 3x + 3
2(x − 1)(x − 3)
)
= limx→3
(
−(x − 3)
2(x − 1)(x − 3)
)
= limx→3
(
−1
2(x − 1)
)
= −1
4
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 27/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(b)
Now applying Formula 2 with f (x) =x
x − 1and a = 3 gives
f ′(3) =
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 28/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(b)
Now applying Formula 2 with f (x) =x
x − 1and a = 3 gives
f ′(3) = limh→0
3 + h
(3 + h) − 1−
3
2
h
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 28/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(b)
Now applying Formula 2 with f (x) =x
x − 1and a = 3 gives
f ′(3) = limh→0
3 + h
(3 + h) − 1−
3
2
h= lim
h→0
1
h
(
3 + h
2 + h−
3
2
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 28/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(b)
Now applying Formula 2 with f (x) =x
x − 1and a = 3 gives
f ′(3) = limh→0
3 + h
(3 + h) − 1−
3
2
h= lim
h→0
1
h
(
3 + h
2 + h−
3
2
)
= limh→0
(
6 + 2h − (6 + 3h)
2h(2 + h)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 28/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(b)
Now applying Formula 2 with f (x) =x
x − 1and a = 3 gives
f ′(3) = limh→0
3 + h
(3 + h) − 1−
3
2
h= lim
h→0
1
h
(
3 + h
2 + h−
3
2
)
= limh→0
(
6 + 2h − (6 + 3h)
2h(2 + h)
)
= limh→0
(
−h
2h(2 + h)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 28/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(b)
Now applying Formula 2 with f (x) =x
x − 1and a = 3 gives
f ′(3) = limh→0
3 + h
(3 + h) − 1−
3
2
h= lim
h→0
1
h
(
3 + h
2 + h−
3
2
)
= limh→0
(
6 + 2h − (6 + 3h)
2h(2 + h)
)
= limh→0
(
−h
2h(2 + h)
)
= limh→0
(
−1
2(2 + h)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 28/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(b)
Now applying Formula 2 with f (x) =x
x − 1and a = 3 gives
f ′(3) = limh→0
3 + h
(3 + h) − 1−
3
2
h= lim
h→0
1
h
(
3 + h
2 + h−
3
2
)
= limh→0
(
6 + 2h − (6 + 3h)
2h(2 + h)
)
= limh→0
(
−h
2h(2 + h)
)
= limh→0
(
−1
2(2 + h)
)
= −1
4
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 28/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(b)
Now applying Formula 2 with f (x) =x
x − 1and a = 3 gives
f ′(3) = limh→0
3 + h
(3 + h) − 1−
3
2
h= lim
h→0
1
h
(
3 + h
2 + h−
3
2
)
= limh→0
(
6 + 2h − (6 + 3h)
2h(2 + h)
)
= limh→0
(
−h
2h(2 + h)
)
= limh→0
(
−1
2(2 + h)
)
= −1
4
Of course, we get the same result using the two formulas. In some
cases the algebra is easier using Formula 1 , but we will use Formula
2 in most cases.
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 28/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) =
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) = limh→0
a + h
(a + h) − 1−
a
a − 1
h
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) = limh→0
a + h
(a + h) − 1−
a
a − 1
h= lim
h→0
1
h
(
a + h
a − 1 + h−
a
a − 1
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) = limh→0
a + h
(a + h) − 1−
a
a − 1
h= lim
h→0
1
h
(
a + h
a − 1 + h−
a
a − 1
)
= limh→0
(
(a + h)(a − 1) − a(a − 1 + h)
h(a − 1)(a − 1 + h)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) = limh→0
a + h
(a + h) − 1−
a
a − 1
h= lim
h→0
1
h
(
a + h
a − 1 + h−
a
a − 1
)
= limh→0
(
(a + h)(a − 1) − a(a − 1 + h)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h −
(
a2− a + ah
)
h(a − 1)(a − 1 + h)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) = limh→0
a + h
(a + h) − 1−
a
a − 1
h= lim
h→0
1
h
(
a + h
a − 1 + h−
a
a − 1
)
= limh→0
(
(a + h)(a − 1) − a(a − 1 + h)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h −
(
a2− a + ah
)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h − a2 + a − ah
h(a − 1)(a − 1 + h)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) = limh→0
a + h
(a + h) − 1−
a
a − 1
h= lim
h→0
1
h
(
a + h
a − 1 + h−
a
a − 1
)
= limh→0
(
(a + h)(a − 1) − a(a − 1 + h)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h −
(
a2− a + ah
)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h − a2 + a − ah
h(a − 1)(a − 1 + h)
)
= limh→0
(
−h
h(a − 1)(a − 1 + h)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) = limh→0
a + h
(a + h) − 1−
a
a − 1
h= lim
h→0
1
h
(
a + h
a − 1 + h−
a
a − 1
)
= limh→0
(
(a + h)(a − 1) − a(a − 1 + h)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h −
(
a2− a + ah
)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h − a2 + a − ah
h(a − 1)(a − 1 + h)
)
= limh→0
(
−h
h(a − 1)(a − 1 + h)
)
= limh→0
(
−1
(a − 1)(a − 1 + h)
)
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c)
Now applying Formula 2 with f (x) =x
x − 1for a general a gives
f ′(a) = limh→0
a + h
(a + h) − 1−
a
a − 1
h= lim
h→0
1
h
(
a + h
a − 1 + h−
a
a − 1
)
= limh→0
(
(a + h)(a − 1) − a(a − 1 + h)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h −
(
a2− a + ah
)
h(a − 1)(a − 1 + h)
)
= limh→0
(
a2− a + ah − h − a2 + a − ah
h(a − 1)(a − 1 + h)
)
= limh→0
(
−h
h(a − 1)(a − 1 + h)
)
= limh→0
(
−1
(a − 1)(a − 1 + h)
)
= −1
(a − 1)2
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 29/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c) – Continued
Substituting a = 3 into the formula for the derivative just derivedgives
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 30/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c) – Continued
Substituting a = 3 into the formula for the derivative just derivedgives
f ′(3) = −1
22= −
1
4
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 30/30
Velocity Rate of Change The Derivative
Example 27 – Calculating a Derivative at a Point
Solution: Example 27(c) – Continued
Substituting a = 3 into the formula for the derivative just derivedgives
f ′(3) = −1
22= −
1
4
which agrees with our calculations in parts (a) and (b).
Clint Lee Math 112 Lecture 7: Velocity and Rate of Change 30/30