Chapter 12: Related Rates
Suppose we have two variables
and
(in most story problems the letters will be different, but for now let's use
and
) which are both changing with time. A ``related rates'' problem is a problem where we know one of the rates of change at a given instant --- say,
/
--- and we want to find the other rate
/
at that instant.
If
is written in terms of
, i.e.,
, then this is easy to do using the chain rule:
=
That is, find the derivative of
, plug in the value of x at the instant in question, and multiply by the given value of dx/dt to get dy/dt.
But often
and
will be related in some other way, for example x =
, or
, or perhaps
, where
and
are expressions involving both variables. In all cases, you can solve the related rates problem by taking d/dt of both sides, plugging in all the known values (namely,
, and dx/dt), and then solving for dy/dt.
Decide what the two variables are.
Find an equation relating them.
Take d/dt of both sides.
Plug in all known values at the instant in question.
Solve for the unknown rate.
Sometimes it may not be convenient or desirable to find the equation between
directly. They might in turn be related to each other by a chain of variables and conditions. We will explain such cases in the examples below.
The radius of a circular puddle is 3 m, and it is increasing at the rate of 1 cm/min. How fast is the puddle's area increasing?
Solution
Here the two things that change with time are: the radius
and the area A. We know
/
= 1 cm/min = 0.01 m/min. We want to find
/
. Thus, in this problem
is playing the role of
, and
is playing the role of
. The relation between the two variables is:
.
Taking d/dt of both sides, we obtain
=
.
Notice that, since we are taking derivatives with respect to
, the derivative of
is
, by the rule for the derivative of a power of a function (the
-rule). In this case we alternately could have used the chain rule for the variables
and
:
.
We now plug in the information given. At the instant in question,
, and
/
=
. Thus,
= (
) (
) (
) =
/
.
Note:
A crucial point to notice in this and similar problems is that, even though a numerical value is given for r, r must be regarded as a variable, not a constant.
The value of the variable at the instant in question cannot be plugged into the equation until
after
taking d/dt of the equation
.
Example 12.2: Spherical Ballon
You are inflating a spherical balloon at the rate of
/
. How fast is its radius increasing at the instant when
? How fast is the area increasing at the same time?
Solution
First we answer the first question.
Here the variables are the radius
and the volume
. We know
/
, and we want
/
. The two variables are related by means of the equation
. Taking
/
of both sides gives
. We now substitute the values we know at the instant in question:
. Solving for
, we obtain
=
cm/sec.
Now the second question.
The formula for the area is
. Taking
/
of both sides, we get
=
.
Now that we have worked out the answer to
/
, we can easily deduce that
/
=
=
.
Note: If only the second question was asked, then we would have first written down the two well known formulas:
,
and tried to find a direct relation between
and
. The relation is
. Then we would try to solve this for
and take derivatives, or take
/
of both sides and finally arrive at the same result.
The point is that it is not necessary to eliminate
right away. It is far easier to take
/
of the two relations first and get equations
,
so
or
.
Our final answer is now clear!
A plane is flying at 500 mph at an altitude of 3 miles in a direction away from where you're standing (i.e., the point on the ground directly beneath the plane is moving away from you). How fast is the plane's distance from you increasing at the moment when the plane is flying over a point on the ground 4 miles from you?
Solution
To see what's going on, we first draw a triangle whose
hypotenuse
is the line from you to the plane (see figure). The vertical leg of the triangle is a constant --- 3 mi --- which does not change in the course of the problem. The horizontal leg
is the variable whose rate we know --- its rate
/
is the speed of the plane. The hypotenuse
is the variable whose rate we want. The equation relating
and
is the
Pythagorean theorem
:
. We next take
/
of both sides, getting
/
=
/
. At the instant in question
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we're told that
and
/
=
. What about
? From the
Pythagorean theorem
, we have:
=
at the instant in question. Thus, we obtain: (2)(4)(500) = (2)(5)
/
, and solving for
/
gives the value
mph. That is, the plane is receding from you at 400 mph. (Until you think about this for a while, it might seem counterintuitive that, although the side
is greater than the side
, its rate of increase is less.)
Example 12.4: Conical Container
Water is poured into a conical container at the rate of
/sec. The cone points directly down (see side view at right), and it has a height of
and a base radius of
. How fast is the water level rising when the water is
deep (at its deepest point)?
Solution
In this problem, the water forms a conical shape within the big cone whose height and base radius --- and hence also its volume --- are all increasing as water is poured into the container. This means that we actually have three things varying with time: the water level
(the height of the cone of water), the radius
of the circular top surface of water (the base radius of the cone of water), and the volume of water V. And we have the relation
. We know
/
, and we want
/
. At first something seems to be wrong: we have a third variable
whose rate we don't know.
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But the dimensions of the cone of water must have the same proportions as those of the container. In other words,
and
fit into the above diagram of similar triangles, from which it follows that
, i.e.,
. So we can eliminate
from the problem entirely:
=
. We now take
/
of both sides and then plug in
and
/
=
, obtaining
. Thus,
/
=
/
=
cm/sec.
Note:
Again we can take the lazy approach and write the equations:
and
that we noticed above. Instead of eliminating the variable
we could have just taken separate derivatives first and then eliminated
/
.
Of course, here the second equation is so easy to solve (it is already solved for
), we did eliminate
right away in our solution. In general, the lazy method is better, unless the elimination is very easy.
A swing consists of a board at the end of a
ft long rope. Think of the board as a point P at the end of the rope, and let Q be the point of attachment at the other end. Suppose that the swing is directly below Q at time
, and is being pushed by someone who walks at the speed of 6 ft/sec from left to right. Find (a) how fast the swing is rising after 1 sec; (b) the angular speed of the rope in deg/sec after 1 sec.
Solution
In doing this problem, we must start out by asking: What is the geometric quantity whose rate of change we know, and what is the geometric quantity whose rate of change we're being asked about? Note that the person pushing the swing is moving
horizontally
at a rate we know. In other words, the
horizontal
coordinate of P is increasing at 6 ft/sec. In the xy-plane let us make the convenient choice of putting the origin at the location of P at time t = 0, i.e., a distance 10 directly below the point Q of attachment. Then the rate we know is
/
.
In part (a) the rate we want is dy/dt (the rate at which P is rising).
In part (b) the rate we want is
, where theta stands for the angle in radians through which the swing has swung from the vertical. (Actually, since we want our answer in deg/sec, at the end we must convert
from rad/sec by multiplying by
.)
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Part (a) :
From the diagram above we see that we have a right triangle whose legs are
and 1
, and whose
hypotenuse
is
. Hence
. Taking
/
of both sides --- and recalling that the derivative of the square of a function of
is twice the function being squared times the time derivative of that function --- we obtain:
+
. We now look at what we know after 1 sec, namely
(because
started at
and has been increasing at the rate of
ft/sec for 1 sec),
(because we get
from the Pythagorean theorem applied to the triangle with hypotenuse
and leg
), and
/
=
. Putting in these values leaves us with (
)
(
)-(
)(
)(
/
) =
, from which we can easily solve for dy/dt, getting dy/dy = 4.5 ft/sec.
Part (b) :
Here our two variables are
and
, so we want to use the same
right triangle as in part (a), but this time to relate
to
. Since the hypotenuse is constant (equal to
), the best way to do this is to use the
:
. Taking
/
of both sides, we obtain (
) (
/
= 0.1
/
. At the instant in question (
sec), when we have a right triangle with sides 6-8-10, the
in this equation is
/
. We also substitute
/
=
on the right. We get 0.8
/
= 0.6, i.e.,
/
=
/
=
rad/sec =
deg/sec.
Sometimes there are
several variables
that change with time, you know the rates of all but one of them, and you want to know the remaining rate. As in the case when there are just two variables, take
/
of both sides of the equation relating all of the variables, and then plug in all of the known values and solve for the unknown rate. In other words, our lazy method is the recommended method!
Example 12.6: Perpendicular Roads
A road going North--South crosses a road going East--West at the point
. Car
is driving North along the first road, and car
is driving East along the second road. At time
car
is
to the North of
, and car
is
to the East of
. Suppose that at some instant you know the values of
, the velocity
of car
, and the velocity
of car
. Find a formula in terms of these known values for the rate at which the distance between the two cars is increasing.
Solution
Let
be the distance from car
to car
. By the Pythagorean Theorem,
. We now take
/
of both sides of the Pythagorean Theorem, obtaining
+
. Dividing by
gives the following formula for the unknown rate:
=
.
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Notice how this problem differs from Example 12.3. In both cases we took
/
of the
Pythagorean Theorem
. However, in Example 12.3 one of the sides was a constant (the altitude of the plane), and so
/
of the square of that side was simply zero. In Example 12.6, on the other hand, all three sides of the right triangle are variables. As always in a story problem, it's important to read the problem carefully enough to determine at the start what are the variables and what are the constants.