I want to see how d/dt (-mu/r) = mu/r^2 * v

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The discussion centers on the differentiation of the expression d/dt [-\mu/r], where r represents the radius, v is the velocity, and \mu is defined as G(M+m). Participants clarify that \mu is a constant and does not change with r, leading to the conclusion that the derivative simplifies to (\mu/r^2) * v. The confusion arises from misapplying the quotient rule and treating \mu as a variable function rather than a constant parameter.

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So here it says that ##d/dt [-\mu/r] = (\mu/r^2)* v ## where ##r## is the separation or radius, and ##v## is the velocity, and ##\mu## is a parameter equal to ##G(M+m)##

And I do not see how they get this to be equal, because all of my tries using the quotient rule create another term that they do not have. Any help will be appreciated :)
 
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AdrianGriff said:
So here it says that ##d/dt [-\mu/r] = (\mu/r^2)* v ## where ##r## is the separation or radius, and ##v## is the velocity, and ##\mu## is a parameter equal to ##G(M+m)##

And I do not see how they get this to be equal, because all of my tries using the quotient rule create another term that they do not have. Any help will be appreciated :)
Do you know what ##\dfrac{d}{dt} f(t)^{-1}## is?
 
fresh_42 said:
Do you know what ##\dfrac{d}{dt} f(t)^{-1}## is?
Haha, no I do not :)
 
AdrianGriff said:
So here it says that ##d/dt [-\mu/r] = (\mu/r^2)* v ## where ##r## is the separation or radius, and ##v## is the velocity, and ##\mu## is a parameter equal to ##G(M+m)##

And I do not see how they get this to be equal, because all of my tries using the quotient rule create another term that they do not have. Any help will be appreciated :)

What do you get when you differentiate that expression?
 
AdrianGriff said:
So here it says that ##d/dt [-\mu/r] = (\mu/r^2)* v ## where ##r## is the separation or radius, and ##v## is the velocity, and ##\mu## is a parameter equal to ##G(M+m)##

And I do not see how they get this to be equal, because all of my tries using the quotient rule create another term that they do not have. Any help will be appreciated :)
The formula above implicitly assumes that r is a function of t. ##\mu## is a constant, since the quantities G, M and m are constants, at least as far as the calculation is concerned.
The quotient rule will work here, and is straightforward to use, if you keep in mind that the derivative of a constant is zero. Please show us what you did, and I'm sure we can set you straight.
 
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PeroK said:
What do you get when you differentiate that expression?
Thank you guys for your support, I will show what I am doing, as I am surely missing something so plainly obvious..

I did use the Quotient Rule also :)
$$\frac {d} {dx} \left[ \frac {g(x)} {h(x)} \right] = \left( \frac {g'(x)h(x) - h'(x)g(x)} {h(x)^2} \right)$$
And thus:
$$\frac {d} {dt} \left[ \frac {-\mu} {r} \right] = \frac {1\mu^0 * r - (-\mu * r')} {r^2} = \frac {r + \mu * v} {r^2}$$

However, @Mark44 's answer tipped me off and I now realize that ##\mu## itself differentiates to 0, and the first term would cancel to zero as well. So thank you.
 
AdrianGriff said:
Thank you guys for your support, I will show what I am doing, as I am surely missing something so plainly obvious..

I did use the Quotient Rule also :)
$$\frac {d} {dx} \left[ \frac {g(x)} {h(x)} \right] = \left( \frac {g'(x)h(x) - h'(x)g(x)} {h(x)^2} \right)$$
And thus:
$$\frac {d} {dt} \left[ \frac {-\mu} {r} \right] = \frac {1\mu^0 * r - (-\mu * r')} {r^2} = \frac {r + \mu * v} {r^2}$$
I'm pretty sure you get it, from what you wrote below, but here's a comment on your work above. It is not true that ##\frac d {dx} \mu = 1\mu^0##. The error here is treating ##\mu## as if it were a function of r. What is correct is that ##\frac d {dr} \mu = 0## -- the derivative of any constant is 0.
AdrianGriff said:
However, @Mark44 's answer tipped me off and I now realize that ##\mu## itself differentiates to 0, and the first term would cancel to zero as well. So thank you.
 
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Mark44 said:
I'm pretty sure you get it, from what you wrote below, but here's a comment on your work above. It is not true that ##\frac d {dx} \mu = 1\mu^0##. The error here is treating ##\mu## as if it were a function of r. What is correct is that ##\frac d {dr} \mu = 0## -- the derivative of any constant is 0.
Thank you :)

However the only ambiguity I can feel for here is that is ##\mu## not a function?
If ##\mu = G(M+m)## is that not considered a function during derivation?
 
AdrianGriff said:
Thank you :)

However the only ambiguity I can feel for here is that is ##\mu## not a function?
If ##\mu = G(M+m)## is that not considered a function during derivation?
No. As you said in post #1, ##\mu## is a parameter, a kind of constant. G is the gravitational constant, and M and m are considered constants for the purpose of differentiation. The only varying quantities are r and ##\frac \mu r##, that latter of which is a function of r.
 
  • #10
Mark44 said:
No. As you said in post #1, ##\mu## is a parameter, a kind of constant. G is the gravitational constant, and M and m are considered constants for the purpose of differentiation. The only varying quantities are r and ##\frac \mu r##, that latter of which is a function of r.
Does treating ##\mu## like a function, and using the chain rule also create the same output? As G, M, and m are all constants and would all derive to be equal to zero? Or must it remain solely as a parameter?

Thank you a lot though :)
 
  • #11
AdrianGriff said:
Does treating ##\mu## like a function, and using the chain rule also create the same output?
No, if I understand what you're asking. Then again, I don't see how the chain rule is applicable in this problem, since another way of writing the function is ##-\mu r^{-1}##, which doesn't call for the chain rule..
In your work you had ##\d {dr} \mu = 1\mu^0 = 1##, which is incorrect.

AdrianGriff said:
As G, M, and m are all constants and would all derive to be equal to zero?
All would differentiate to zero, yes. (We don't say "derive" when we differentiate something.) You can derive the Quadratic Formula when you solve a quadratic equation by completing the square, but you differentiate ##\sin(x)## to get ##\cos(x)##.
 
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  • #12
AdrianGriff said:
Thank you :)

However the only ambiguity I can feel for here is that is ##\mu## not a function?
If ##\mu = G(M+m)## is that not considered a function during derivation?

You can consider it a function of time, but it's a constant function. If you draw a graph of ##G(M+m)## against time, the graph is flat, so the derivative is ##0##.

More fundamentally, though, you shouldn't even be trying to differentiate constants like that.
 
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