How fast is the radius of the basketball increasing when the radius is 16 cm if air is being pumped into a basketball at a rate of 100 cm3/sec?

Answer 1
In mathematicsland, basketballs are perfect spheres with #0# thickness (inside radius = 0utside radius).
Air is being pumped in at a rate of #100 " cm"^3"/sec"#.
This rate of change is a rate of change of something with respect to some (other) thing. We expect related rates (of change) problems to involve derivatives with respect to time, #t#.
So, we expect to see a #(d("something"))/(dt)#.
Now, #" cm"^3"# is a measure of volume, so we see that we have:
#(dV)/dt = 100 " cm"^3"/sec" #
We are asked to find how fast radius, #r# is changing, that is, we are asked to find #(dr)/dt# when #r = 16" cm"#.
We need an equation with #V# and #r#. For a sphere,
#V=4/3 pir^3#
We understand that both #V# and #r# are functions of the (unmentioned) variable #t#. We will differentiate with respect to #t#:
#d/dt(V)= d/dt(4/3 pir^3)#
#(dV)/dt= 4/3 pi *3r^2 (dr)/dt# (In implicit differentiation, we use the chain rule.)
#(dV)/dt= 4 pi r^2 (dr)/dt#

Now, plug in what we know and solve for what we don't know:

#100 " cm"^3"/sec" = 4 pi (16" cm")^2 (dr)/dt#
So #(dr)/dt = 100/(4 pi 16^2) (" cm"^3"/sec")/" cm"^2#
#(dr)/dt = 25/( pi 16^2) " cm/sec"#

Do whatever arithmetic you like or are required to do to get the answer in an acceptable form.

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Answer 2

To find the rate at which the radius of the basketball is increasing, we can use the formula relating the volume ( V ) of a sphere to its radius ( r ):

[ V = \frac{4}{3}\pi r^3 ]

Taking the derivative of both sides with respect to time ( t ), we get:

[ \frac{dV}{dt} = 4\pi r^2 \frac{dr}{dt} ]

Given that the volume is increasing at a rate of ( \frac{dV}{dt} = 100 ) cm³/s when the radius ( r = 16 ) cm, we can plug in these values into the equation and solve for ( \frac{dr}{dt} ), the rate at which the radius is increasing:

[ 100 = 4\pi (16)^2 \frac{dr}{dt} ] [ \frac{dr}{dt} = \frac{100}{4\pi (16)^2} ] [ \frac{dr}{dt} = \frac{100}{4\pi \times 256} ] [ \frac{dr}{dt} = \frac{100}{1024\pi} ] [ \frac{dr}{dt} ≈ \frac{100}{3207} ] [ \frac{dr}{dt} ≈ 0.0312 , \text{cm/s} ]

Therefore, the radius of the basketball is increasing at a rate of approximately ( 0.0312 ) cm/s when the radius is 16 cm.

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Answer from HIX Tutor

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.

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