Global extrema without numbers

In summary, when coughing, the speed of air coming out depends on the radius of the windpipe, with a maximum speed given by v = a(R-r)r2 where R is the normal radius and r is the radius of the windpipe. To find the maximum speed, the derivative of the function is set equal to 0 and solved for r, resulting in r = (2/3)R. This value is then plugged back into the original function to find the maximum speed. The procedure for finding global extrema is to find function values at all critical points and endpoints, and in this case, the maximum speed is found at r = (2/3)R.
  • #1
Razael
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0

Homework Statement



When you cough, your windpipe contracts. The speed, v, with which air comes out depends on the radius, r, of your windpipe. If R is the normal (rest) radius of your windpipe, then for r <_ R, the speed if given by v = a(R-r)r2 where a is a positive constant. What value of r maximizes v? What is the maximum speed? Show all work. Use the procedure for finding global extrema to justify that you have found the global maximum velocity.

Homework Equations



v = a(R-r)r2

The Attempt at a Solution



Derivative is 2ar(R-r) - ar2 (R is considered a constant, right?)

= 2arR - 2ar2 -ar2

= 2arR - 3ar2 = 0

2arR = 3ar2

2aR = 3ar

r = (2/3)R

Not too confident in that answer. For maximum speed I just plugged it into the original equation:

v = a((2/3)R)2((1/3)R)

Any help is appreciated, whether it be by pointing out a mistake or helping with the last part (justify answer).

Edit The interval would be 0 < r <_ R, right?
 
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  • #2
(You've assumed that r is nonzero in your calculuation. Do you know where?)


Not sure if this is right? Well, let's look at what you've proven:

If v = a(R-r)r², and a and R are constants w.r.t. r, then dv/dr = 0 if and only if r = (2/3) R. (Assuming r is nonzero)

Well, that wasn't what you were trying to show now, is it? You were trying to say something about extrema, not zeros of derivatives! You need to add something to your argument. It might be a minor thing, but it needs to be added.


P.S. what is "the procedure for finding global extrema"?
 
  • #3
Hurkyl said:
(You've assumed that r is nonzero in your calculuation. Do you know where?)

Here?

2arR = 3ar2

2aR = 3ar

Now that I think about it, r could be 0 (I assumed breathing was occurring :blushing:)


Not sure if this is right? Well, let's look at what you've proven:

If v = a(R-r)r², and a and R are constants w.r.t. r, then dv/dr = 0 if and only if r = (2/3) R. (Assuming r is nonzero)

Well, that wasn't what you were trying to show now, is it? You were trying to say something about extrema, not zeros of derivatives! You need to add something to your argument. It might be a minor thing, but it needs to be added.

It said extrema so I assumed I'd be finding critical points. Am I going about that wrong?


P.S. what is "the procedure for finding global extrema"?

Finding function values at all critical points and endpoints.
 
  • #4
Just to clarify, r <_ R means r is less or equal to R.
 
  • #5
Razael said:
Here?

2arR = 3ar2

2aR = 3ar

Now that I think about it, r could be 0 (I assumed breathing was occurring :blushing:)
Yep.

It said extrema so I assumed I'd be finding critical points. Am I going about that wrong?
...
Finding function values at all critical points and endpoints.
Mainly, I wanted to make sure you didn't mentally replace "find the extrema" with "find where the derivative is zero".

The procedure you cite here is a reasonable one for finding extrema. And you are executing the "find the critical points" bit correctly. But from your original post, I couldn't tell if you knew why you were finding the critical points, or if you were going to remember to check the endpoints.
 
  • #6
I assumed r wasn't 0 because doing so would make v 0 (which wouldn't be a maximum). So I ended up with two local maxes; (2/3)R and R (the right end of the interval).

So now I put these values into the original function and find which results in a higher value, correct?

Edit: Using interval-end R as a value of r results in a function value of 0. (2/3)R is all I'm left with.
 
  • #7
Razael said:
So now I put these values into the original function and find which results in a higher value, correct?
If that's what the theorem about global maxima that you're using says, then yes, that's what you do!

I assumed r wasn't 0 because doing so would make v 0 (which wouldn't be a maximum). So I ended up with two local maxes; (2/3)R and R (the right end of the interval).
A minor digression: while R is a local extremum, you haven't shown it to be a maximum. In fact, it can't be a local maximum: between any two local maxima, there must be a local minimum!
 
  • #8
Hurkyl said:
A minor digression: while R is a local extremum, you haven't shown it to be a maximum. In fact, it can't be a local maximum: between any two local maxima, there must be a local minimum!

Good point. Both r=0 and r=R result in the function equaling 0, so I guess they would both be minimums while r=(2/3)R would be the maximum (so it'd look like a concave down parabola).

Thanks for the help :smile:
 

FAQ: Global extrema without numbers

1. What are global extrema?

Global extrema are the maximum and minimum values of a function over its entire domain.

2. How are global extrema different from local extrema?

Local extrema are the maximum and minimum values of a function within a specific interval or region, while global extrema are the maximum and minimum values over the entire domain of the function.

3. Can a function have more than one global extremum?

Yes, a function can have multiple global extrema if its graph has multiple peaks and valleys over its entire domain.

4. How can global extrema be identified without numbers?

Global extrema can be identified by analyzing the shape of the graph of a function and looking for the highest and lowest points over its entire domain.

5. Are global extrema always present for every function?

No, not all functions have global extrema. Some functions may have infinite or no global extrema, depending on their domain and range.

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