Power output by basketball player when jumping

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The discussion revolves around calculating the power output of a basketball player during a jump, specifically focusing on the acceleration phase. The player exerts a force while crouching and then jumps, with calculations showing a power output of 7.49 kW, which differs from the textbook's answer of 8.93 kW. The discrepancy arises from the method of calculating time, with the textbook adding gravitational acceleration to the player's acceleration, which some participants argue is incorrect. The conversation also touches on the complexities of modeling real-life scenarios involving variable acceleration and the challenges of deriving a closed-form solution for constant power output. Ultimately, the participants express confusion over the correct approach to these physics problems and the implications of constant versus average power calculations.
Jazz
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Homework Statement



A ##\small{105\!-\!kg}## basketball player crouches down ##\small{0.400\ m}## while waiting to jump. After exerting a force on the floor through this ##\small{0.400\ m}##, his feet leave the floor and his center of gravity rises ##\small{0.950\ m}## above its normal standing erect position.

What was his power output during the acceleration phase?

##m = 105\ kg##

##d = 0.400\ m##

##h = 0.950\ m##

Homework Equations



##P = \frac{W}{t}##

##\Delta PE_g = \Delta KE##

The Attempt at a Solution



The problem disregards the work done by the player when first crouches, so the work I tried to find is just when he accelerates upwards (jumps).

First we know that: ##P_{output} = \frac{W_{output}}{t} = \frac{F_{exerted}d}{t}##

The velocity with which he left the floor is the same to that just before he touches the floor when landing; and after having fallen a height ##h##:

##\Delta PE_g = \Delta KE##

##mgh = \frac{1}{2}mv^2##

##v= \sqrt{2gh} = \sqrt{(2)(9.8\ m/s^2)(0.950\ m)} = 4.32\ m/s##Assuming that the velocity was obtained after a net constant acceleration along a distance ##d##, then:

##a = \frac{v^2}{2d} = \frac{2gh}{2d} = \frac{(9.8\ m/s^2)(0.950\ m)}{0.400\ m} = 23.3\ m/s^2##Then, I try to find the average force exerted:

##F_{exerted} = F_{net} + w##

##F_{exerted} = m(a + g)##

##F_{exerted} = (105\ kg)[23.3\ m/s^2 + 9.8\ m/s^2] = 3473\ N##Then, I tried to find the time:

##t = \frac{v-v_0}{a} = \frac{4.32\ m/s}{23.3\ m/s^2} = 0.185\ s##And finally the power:

##P_{output} = \frac{F_{exerted}d}{t} = \frac{(3473\ N)(0.400\ m)}{0.185\ s} = 7.49\ kW##

But the answer provided by the textbook says that the power must be ##8.93\ kW##. After playing around with the numbers, I noticed that what makes the difference between both results is the way the time was calculated. According to the textbook, the time is:

##t= \sqrt{\frac{2d}{(a + w)}} = \sqrt{\frac{2(0.400\ m)}{(23.3\ m/s^2 + 9.8\ m/s^2)}} = 0.156\ s##

My question is: why should ##g## be added to the ##a##? It's like considering an absolute acceleration exerted by the player, but that should underestimate the time the force was exerted.

In a hypothetical situation, if I were pushing a box with an acceleration of ##1\ m/s## through a distance ##d##, and it happens that I know friction is exerting an acceleration of ##3\ m/s## in the opposite direction, the time I spent pushing the box is dependent of ##a## but not ##a + a_{friction}##. The latter will yield a shorter time than that I really spent pushing the box (and hence, a greater power output).

I'm puzzled.
 
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Hi Jazz. You have presented your case well. I agree with you that the textbook solution is wrong.
 
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The question does not make it clear that the force is constant, while the power to be determined is an average. If that is correct I agree with your answer.
More realistically for muscle, power is constant. But that leads to quite a messy equation, with no solution in closed form.
 
Thank you, both, for your answers.

haruspex said:
The question does not make it clear that the force is constant, while the power to be determined is an average. If that is correct I agree with your answer.
More realistically for muscle, power is constant. But that leads to quite a messy equation, with no solution in closed form.

The problems involving force that I've been dealing with so far just consider average acceleration. I know that this does not happen in real life (at least not in situations as in the problem) but I get very confused trying to understand how a problem with changing acceleration must be treated (as far as I understand, with help of calculus I will be able to do so).

In this case, if I were asked to find a constant power output, does it mean that the magnitude of the force gets reduced, but the time over which it acts gets longer along the distance ##d##, 'fitting' an equation like this ##\frac{\Delta F}{\Delta t}d##?

If there is no closed form for calculating constant power, is it calculated by taking shorter distances ##d## along which a force ##F## acts during a time ##t## and then add them, or by taking shorter times over which it acts and add them?

If I were asked to find
 
Last edited:
Jazz said:
Thank you, both, for your answers.
The problems involving force that I've been dealing with so far just consider average acceleration. I know that this does not happen in real life (at least not in situations as in the problem) but I get very confused trying to understand how a problem with changing acceleration must be treated (as far as I understand, with help of calculus I will be able to do so).

In this case, if I were asked to find a constant power output, does it mean that the magnitude of the force gets reduced, but the time over which it acts gets longer along the distance ##d##, 'fitting' an equation like this ##\frac{\Delta F}{\Delta t}d##?

If there is no closed form for calculating constant power, is it calculated by taking shorter distances ##d## along which a force ##F## acts during a time ##t## and then add them, or by taking shorter times over which it acts and add them?

If I were asked to find
Not sure you've understood what I mean by 'no closed form'. Using calculus, you get an equation for P which involves P in 'incompatible' ways. Specifically, I got ##mg(d+h) = -P\sqrt{\frac{2h}{g}} - \frac{P^2}{mg^2}\ln\left(1-\frac {mg}{P}\sqrt{2gh}\right)## , but that's so horrible I suspect I made an error. At least it's dimensionally correct.
 
haruspex said:
Not sure you've understood what I mean by 'no closed form'. Using calculus, you get an equation for P which involves P in 'incompatible' ways. Specifically, I got ##mg(d+h) = -P\sqrt{\frac{2h}{g}} - \frac{P^2}{mg^2}\ln\left(1-\frac {mg}{P}\sqrt{2gh}\right)## , but that's so horrible I suspect I made an error. At least it's dimensionally correct.

Roughly speaking, I understood a closed form as a nice formula used to solve 'something' that seems to be messy. Maybe it's too rough.

I hope to get into the math soon to understand how to get the equation you got. Just for curiosity, ##mg(d+h)## is considering the distance he crouches, why is that?

So when considering constant P, both I and the textbook are wrong, right?
 
Jazz said:
##mg(d+h)## is considering the distance he crouches, why is that?
That's the total work done, no?
Jazz said:
So when considering constant P, both I and the textbook are wrong, right?
Without completely solving it, I can't be certain it won't give the textbook answer, but it seems unlikely. As I wrote, my equation could be wrong.
 
haruspex said:
That's the total work done, no?

Yep, I was just overthinking about it.

haruspex said:
Without completely solving it, I can't be certain it won't give the textbook answer, but it seems unlikely. As I wrote, my equation could be wrong.

(:

Thanks for helping me to see the light with this.
 

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