Chapter 34 Instantaneous Rates of Change An important goal for this course is to understand not only how to find derivatives for example but also to understand the derivative as a concept Its easy to know how to find the derivative of say ID: 275045
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Slide1
Velocity and Other Rates of Change
Chapter 3.4Slide2
Instantaneous Rates of Change
An important goal for this course is to understand, not only how to find derivatives, for example, but also to understand the derivative as a concept
It’s easy to know how to find the derivative of, say,
; it’s more challenging and more useful to also know how to interpret the derivative of (in general and in specific instances)In this section we will develop the concept of instantaneous rate of change by first looking at position, velocity, and acceleration as archetypes of this conceptAn archetype is “a statement, pattern of behavior, or prototype which other statements, patterns of behavior, and objects copy or emulate”*
*https://en.wikipedia.org/wiki/Archetype
2Slide3
Instantaneous Rates of Change
By “understanding instantaneous rate of change conceptually” is meant that you are able to understand and interpret
The derivative of a function analytically (i.e., when you take a derivative)
The derivative of a function from its graph (or the function from a graph of its derivative)The derivative of a function from a table of dataThe derivative of a function from a verbal description of the data3Slide4
Instantaneous Rate of Change
We earlier defined instantaneous rate of change of a function
at some
as
This is the same as finding the derivative of
at a function, then evaluating the derivative at
The result tells us how the function value is changing with respect to
at
It is also the same as the slope of the tangent line at
4Slide5
Instantaneous Velocity
DEFINITION:
The
instantaneous velocity is the derivative of the position function with respect to time, . At time the instantaneous velocity is
5Slide6
Displacement and Instantaneous Velocity
DEFINITIONS:
Let
be a position function. Then:The displacement of a moving object over the time interval from to is
The
average velocity
of the object over the time interval is
6Slide7
Instantaneous Velocity
Comparison: if
is a position function, then
The displacement over a time interval from to is
The
average velocity
over a time interval from
to
is
The instantaneous velocity
at a time
is
7Slide8
Instantaneous Velocity
To find the velocity of the object at an exact instant
, we take the limit of the average velocity as
, which is just the derivativeNote that the units for are units of position (inches, feet, meters, miles, and so on)The units for are units of time (seconds, minutes, hours, days, and so on)
So the units for both average velocity and instantaneous velocity are units of position per unit of time (feet per second, miles per hour, etc.)
8Slide9
Example 2: Vertical Motion
Suppose that an object is thrown vertically from initial position
feet with initial velocity
feet per second. Since the acceleration due to gravity is approximately feet per second per second, then the position function for the object is
. What is the average velocity over the interval
? What is the instantaneous velocity at
seconds?
9Slide10
Example 2: Vertical Motion
10Slide11
Speed
Velocity is a vector quantity, meaning that it has both magnitude and direction
When movement is either vertical or horizontal (with respect to some axes), then velocity is either positive or negative
With our usual axes, velocity is positive when movement is upward and negative when movement is downwardHorizontally, velocity is positive when movement is to the right and negative when movement is to the leftThe speed of an object is the value of the velocity without regard to direction11Slide12
Speed
DEFINITION:
Speed
is the absolute value of velocity
12Slide13
Example 3: Reading a Velocity Graph
A student walks around in front of a motion detector that records her velocity at 1-second intervals for 36 seconds. She stores the data in her graphing calculator and uses it to generate the time-velocity graph shown below. Describe her motion as a function of time by reading the velocity graph. When is her
speed
a maximum?13Slide14
Example 3: Reading a Velocity Graph
She walks forward (away from the detector) for the first 14 seconds, moves backward for the next 12 seconds, stands still for 6 seconds, and then moves forward again. Her maximum speed occurs at about 20 seconds, while walking backward.
14Slide15
Acceleration
DEFINITION:
Acceleration
is the derivative of velocity with respect to time. If a body’s velocity at time is , then the body’s acceleration at time
is
or
15Slide16
Acceleration Due to Gravity
The Earth’s gravity “pulls” objects towards its center with a constant (near the surface) acceleration
The variable
is often used to represent this accelerationIn English units: feet per second per second;
In metric units:
meters per second per second;
16Slide17
Example 4: Modeling Vertical Motion
A dynamite blast propels a heavy rock straight up with a launch velocity of 160 feet per second. It reaches a height of
after
seconds.How high does the rock go?
What is the velocity and speed of the rock when it is 256 ft above the ground on the way up? on the way down?What is the acceleration of the rock at any time
during the flight?When does the rock hit the ground?
17Slide18
Example 4: Modeling Vertical Motion
How high does the rock go?
You should recognize that the position function is a quadratic function and its graph is a parabola opening down. This means that it must have a maximum value which occurs at the vertex and we could use the vertex formula to find the time at which it reaches its maximum height. But it is also the case that, at this instant, the rock has zero velocity. So using calculus we can find the velocity function:
Now,
seconds
18Slide19
Example 4: Modeling Vertical Motion
What is the velocity and speed of the rock when it is 256 ft above the ground on the way up? on the way down?
Find the times when the rock is 256 feet above the ground by solving for
:
On the way up the velocity is
feet per second; speed 96 ft/sec
On the way down the velocity is
feet per second; speed 96 ft/sec
19Slide20
Example 4: Modeling Vertical Motion
What is the acceleration of the rock at any time
during the flight?
Acceleration is the second derivative of the position function:
The acceleration is a constant 32 feet per second per second towards the Earth.
20Slide21
Example 4: Modeling Vertical Motion
When does the rock hit the ground?
At ground level, the position function equals zero (and this must occur twice).
The rock returns to the ground after 10 seconds.
21Slide22
Example 5: Studying Particle Motion
A particle moves along the
-axis so that its position at any time
is given by the function
, where
is measured in meters and
is measured in seconds.
Find the displacement of the particle during the first 2 seconds.
Find the average velocity of the particle during the first 4 seconds.
Find the instantaneous velocity of the particle when
.
Find the acceleration of the particle when .Describe the motion of the particle. At what values of does the particle change directions? 22Slide23
Example 5: Studying Particle Motion
Find the displacement of the particle during the first 2 seconds.
We have defined displacement to be the value
, where
for this problem. So the displacement is
Note that displacement gives the distance and direction (by means of the sign) that the particle moved
from its start position
. A separate but related question that we will encounter later is, what is its new position on the
-axis?
23Slide24
Example 5: Studying Particle Motion
Find the average velocity of the particle during the first 4 seconds.
By definition
24Slide25
Example 5: Studying Particle Motion
Find the instantaneous velocity of the particle when
.
Instantaneous velocity is the derivative of at
so
25Slide26
Example 5: Studying Particle Motion
Find the acceleration of the particle when
.
By definition
The acceleration is constant at 2 meters per second per second
26Slide27
Example 5: Studying Particle Motion
Describe the motion of the particle. At what values of
does the particle change directions?
The graph of is a parabola that opens up. So the particle will move downward until it reaches the vertex point, then it will continue upward. At the vertex, it will have stopped moving for an instant, so its velocity there must be zero. We can find the vertex point by solving for in the velocity function:
So for
, the particle moves to the left, and for
it moves right.
27Slide28
Example 6: Enlarging Circles
Find the rate of change of the area
of a circle with respect to its radius
.Evaluate the rate of change of at and at
If is measured in inches and
is measured in square inches, what units would be appropriate for
?
28Slide29
Example 6: Enlarging Circles
Find the rate of change of the area
of a circle with respect to its radius
.The wording above is important: you are being asked to find the derivative of with respect to , or
29Slide30
Example 6: Enlarging Circles
Evaluate the rate of change of
at
and at Find and
Note that the rate of change increases as the radius increases. The same change in
produces a correspondingly greater change in
. That is, the area is increasing much faster than the radius.
30Slide31
Example 6: Enlarging Circles
31Slide32
Example 6: Enlarging Circles
32Slide33
Example 6: Enlarging Circles
If
is measured in inches and
is measured in square inches, what units would be appropriate for ?Notice the analogy here to velocity versus position. That is, given a position function, the independent values are units of time while the dependent (function) values are those of distance. So the units of the derivative are units of distance per unit of time. By analogy in this case, the independent values are those of length while the dependent (function) values are of area. So the units for the derivative are square inches of area per inch of radius.
33Slide34
Derivatives in Economics
The previous example showed how we can use the relationship between position and velocity to understand the relationship between area and radius in an expanding circle
What follows next is a similar analogy, this time in economics
In a manufacturing operation, the cost of production, , is a function of , the number of units producedThe marginal cost of production is the rate of change of cost with respect to level of production (that is, with respect to the number of units produced)What should be the units of marginal cost of production?
34Slide35
Derivatives in Economics
Let’s develop the idea of marginal cost in the same way we developed instantaneous velocity (we could call marginal cost “instantaneous cost”)
Economists often think of marginal cost as the cost of producing one more item (because individual items are not infinitely divisible)
So, if is the cost of producing items, then is the cost of producing
itemsThe average cost of producing one more item is thus
35Slide36
Derivatives in Economics
The average cost of producing one more item is thus
Marginal cost is actually a way of approximating the producing of “one more item” by using the derivative of
when
is much larger than 1
That is,
36Slide37
Example 7: Derivatives in Economics
Suppose a company has estimated that the cost (in dollars) of producing
items is
. What is the marginal cost of producing 500 items? What is the actual cost of producing 1 more item (i.e., the 501st item)?
37Slide38
Example 7: Derivatives in Economics
Since marginal cost is the derivative of the cost function, then
The cost of producing 1 more item is
We see that the marginal cost is close to the actual cost.
38Slide39
Linear Density
If a rod is homogeneous, then its mass is distributed equally along its length
Its linear density is uniform and defined as mass per unit length,
, and the units are kilograms per meter (the symbol is the Greek letter rho)If the rod is not homogeneous, then its mass changes along its length (think of a conical rod) and the mass from its left end to some point is
39Slide40
Linear Density
If we pick two points along the rod at distances
and
from the left (with
, then the average density for this section of the rod is
If we now let
(that is, let
), then we can find the linear density at
Note that the units are still in mass per unit distance from the left
40Slide41
Example 8: Linear Density
Suppose that the mass of a rod varies with distance from its left end such that
, where
is in meters and
is kilograms. What is the average density of the rod for
? What is the density at
meter?
41Slide42
Example 8: Linear Density
The
average density for the interval
is
The linear density at
meters is
So
42Slide43
Exercise 3.4
Online exercise
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