Can I undo a derivative to solve for a variable?

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Discussion Overview

The discussion revolves around the process of undoing a derivative to solve for a variable, particularly in the context of physics equations involving force and momentum. Participants explore the mathematical and conceptual aspects of derivatives and integrals, with a focus on how to manipulate equations to isolate variables.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest that to solve for a variable surrounded by a derivative, one can think backwards to find a function whose derivative matches the given constant.
  • Others argue that the relationship between variables must be clarified, particularly whether certain quantities are constants or functions of time.
  • A participant raises a specific physics question regarding the equation F = dp/dt, expanding momentum into m*v*λ-½, and expresses uncertainty about isolating v from this derivative expression.
  • Another participant mentions that λ may also depend on v, complicating the relationship further.
  • Some participants discuss the need to solve a differential equation derived from the original equation, indicating that the solution involves integrating to find v as a function of time.
  • There is a mention of antiderivatives and their role in reversing derivatives, with some participants questioning how to apply this concept to variables.
  • One participant expresses confusion about taking the integral of a variable and how to handle it mathematically.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the best approach to isolate the variable v from the derivative expression. Multiple competing views and methods are presented, with ongoing questions and clarifications regarding the relationships between the variables involved.

Contextual Notes

There are limitations in the discussion regarding the assumptions about constants and functions, as well as the specific definitions of the variables involved. The discussion also reflects varying levels of familiarity with calculus concepts, particularly derivatives and integrals.

Who May Find This Useful

This discussion may be useful for beginners in physics and mathematics who are trying to understand the relationship between derivatives and integrals, particularly in the context of solving equations involving motion and forces.

Intle
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If I have an equation where there is a derivative surrounding the variable, how do I undo the derivative and solve for the variable?

Example would be-
A= dx/dy when x=m*v*λ-2 and y=y
Solving for v.

I am a beginner so please explain thoroughly.
 
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Intle said:
If I have an equation where there is a derivative surrounding the variable, how do I undo the derivative and solve for the variable?

Example would be-
A= dx/dy when x=m*v*λ-2 and y=y
Solving for v.

I am a beginner so please explain thoroughly.
It's not clear what dx/dy means when there is no explicit relationship between x and y.

If you want to solve for v in the equation above, that can be done using simple algebra.
 
Since dx/dy = A, there is some function x whose derivative with respect to y is the constant A. So think backwards: what function of y has the constant A as its derivative with respect to y?

Then since x will be equal to this this function and also x = m*v*λ2, set the function you found by working backwards from the derivative equal to m*v*λ2 and solve for v using basic algebra.
 
jack476 said:
Since dx/dy = A, there is some function x whose derivative with respect to y is the constant A. So think backwards: what function of y has the constant A as its derivative with respect to y?

Then since x will be equal to this this function and also x = m*v*λ2, set the function you found by working backwards from the derivative equal to m*v*λ2 and solve for v using basic algebra.
I'm afraid I'm not following your train of thought. My question actually was more of a physics question; however the equation I was referring to had derivatives in it and I wanted to know how to undo them. What I typed above was an example; however I now see that that may have let to confusion of what I was asking. So the equation I want to solve is,-
Force = the derivative of momentum with respect to time. So it would look like this- F=dp/dt. However p, or momentum can be expanded into, m*v*λ. I would like to solve for v, but I don't know how to get it out of this derivative expression. I have not yet taken calculus so that's why I am asking.
 
Intle said:
I'm afraid I'm not following your train of thought. My question actually was more of a physics question; however the equation I was referring to had derivatives in it and I wanted to know how to undo them. What I typed above was an example; however I now see that that may have let to confusion of what I was asking. So the equation I want to solve is,-
Force = the derivative of momentum with respect to time. So it would look like this- F=dp/dt. However p, or momentum can be expanded into, m*v*λ. I would like to solve for v, but I don't know how to get it out of this derivative expression. I have not yet taken calculus so that's why I am asking.
Isn't it so that λ also contains v: that λ=1-v2/c2?
 
Before solving something you must decide what are constants or not. For example in your example the velocity ##v## can be view as a function of the time, the same for ##\lambda## (if ## \lambda=1-\frac{v^2}{c^2}##), and assuming constant mass, you equation will be:

##F=m\frac{d}{dt}\left(\frac{v(t)}{\sqrt{1-\frac{v(t)^2}{c^2}}}\right).##

If ## \lambda## is constant the equation will be much simple ## \frac{F}{m}\lambda^{\frac{1}{2}}=\frac{d}{dt}v(t) ##.
 
Ssnow said:
Before solving something you must decide what are constants or not. For example in your example the velocity ##v## can be view as a function of the time, the same for ##\lambda## (if ## \lambda=1-\frac{v^2}{c^2}##), and assuming constant mass, you equation will be:

##F=m\frac{d}{dt}\left(\frac{v(t)}{\sqrt{1-\frac{v(t)^2}{c^2}}}\right).##

If ## \lambda## is constant the equation will be much simple ## \frac{F}{m}\lambda^{\frac{1}{2}}=\frac{d}{dt}v(t) ##.
So if i follow your work correctly I see that you put all of the constants out of the derivative expression and then just used algebra to get the constants to the other side. But doesn't the final answer still contain one unknown, the t, and there still is a v in the λ expression (I apologize for not clarifying, it's not a constant). Also, why did you put a t in parentheses by the v, is this some sort of notation?
 
So you must to solve this differential equation:

## F=m\frac{d}{dt}\left(\frac{v(t)}{1-\frac{v^2(t)}{c^2}}\right)##

that gives you ##\frac{v(t)}{1-\frac{v^2(t)}{c^2}}=\frac{F}{m}t+c## with ##c## a constant. From this you can find ##v(t)## with algebraic operations...
 
Ssnow said:
So you must to solve this differential equation:

## F=m\frac{d}{dt}\left(\frac{v(t)}{1-\frac{v^2(t)}{c^2}}\right)##

that gives you ##\frac{v(t)}{1-\frac{v^2(t)}{c^2}}=\frac{F}{m}t+c## with ##c## a constant. From this you can find ##v(t)## with algebraic operations...
Alright, can you show me how you got to that point?
 
  • #10
you have that ##\frac{F}{m}=\frac{d}{dt}\left(\frac{v(t)}{1-\frac{v^{2}(t)}{c^2}}\right)## so integrating the constant ##\int \frac{F}{m} d\,t=\frac{F}{m}t+c##.
 
  • #11
Are you familiar with anitderivatives? The derivative take you one way and the antiderivative take you the other way. This is what Ssnow is trying to show you.
 
Last edited:
  • #12
zAbso said:
Are you familiar with anitderivatives? The derivative take you one way and the antiderivative take you the other way. This is what Ssnow is trying to show you.
I understand the concept of an anti derivative, that it undoes a derivative and that it is an integral I believe. So the integral of 2x would be x2, yeah iI understand the "reverse operation"; however, I don't understand how you can take the integral, or the anti derivative of a a variable.
 
  • #13
Intle said:
I don't understand how you can take the integral, or the anti derivative of a a variable.
Are you asking if you just have x, how do you get the antiderivative?
For something like 2x you would break it apart to 2∫xdx, which would then become 2 ∫ (xn+1/n+1)

so 2∫xdx would break down to 2 ∫ (x1+1/1+1)
2 ∫ (x2/2)
put it back together for 2x2/2
You would then do your cancellations, equaling x2

for just x focus on the xn+1/n+1,
remember that it's always understood to be x1 for any variable that doesn't have a superscript written and simply plug in 1 for n
So you would get x1+1/1+1, which would come out to x2/2 with nothing to cancel
 
  • #14
If we assume that F and m are constants and that v is a function of t, then the solution is as Ssnow wrote.
 

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