Velocity from acceleration if acceleration is a function of space

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Discussion Overview

The discussion revolves around the implications of defining acceleration as a function of space, a(x), rather than time, a(t). Participants explore how to derive velocity as a function of space, v(x), through integration and the use of the chain rule, while addressing the relationship between velocity and time.

Discussion Character

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

Main Points Raised

  • Some participants propose that integrating a(x) dx could yield velocity as a function of space, v(x), but question the validity of this approach since acceleration is typically defined as a time derivative.
  • One participant outlines a derivation using the chain rule, leading to the equation v dv = f(x) dx, and suggests that if f(x) can be integrated, it results in a relationship between velocity and position.
  • There is a discussion about whether velocity should be treated as a function of time, v(t), or space, v(x), with some arguing that v(x) is appropriate in this context.
  • Participants express confusion about the nature of acceleration as a function of space and its relationship to time derivatives, leading to questions about the correctness of different formulations.
  • One participant mentions that while both a(x) = dv(x)/dt and a(t) = dv(t)/dt can be correct, defining acceleration as a function of x may complicate finding a corresponding time-based equation.
  • Another participant emphasizes that it is mathematically permissible to differentiate a function with respect to a different variable, relating this to the chain rule.

Areas of Agreement / Disagreement

Participants express differing views on the treatment of velocity and acceleration as functions of time versus space. The discussion remains unresolved, with no consensus on the implications of defining acceleration as a function of space.

Contextual Notes

Participants highlight the potential limitations of their approaches, including the dependence on specific forms of acceleration and the challenges in deriving time-based equations from spatial definitions.

fisico30
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Hello Forum,

usually the acceleration a is a function of time: a(t)= d v(t) /dt

to find v(t) se simply integrate v(t)= integral a(t) dt

What if the acceleration was a function of space, i.e. a(x)?

what would we get by doing integral a(x) dx? The velocity as a function of space, v(x)?

but a(x) is not defined to be v(x)/dx or is it? maybe some chain rule is involved..

thanks,

fisico30
 
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fisico30 said:
What would we get by doing integral a(x) dx? ... chain rule ...
You use chain rule

a(x) = dv/dt = f(x)

multiply dv/dt by dx/dx:

(dv/dt)(dx/dx) = (dx/dt)(dv/dx) = v dv/dx = f(x)

multiply both sides by dx

v dv = f(x) dx

If f(x) can be integrated and the integral of f(x) = g(x), then

1/2 v2 = g(x) + c

This results in an equation that relates velocity and position.

v = sqrt(2 (g(x) + c))

To get time versus position, you start with

v = dx/dt = sqrt(2 (g(x) + c))

and then integrate

dx/(sqrt(2 (g(x) + c))) = dt

assuming h(x) is the integral of dx/(sqrt(2 (g(x) + c))), you get

t = h(x) + d

where d is constant of integration. It may be possible to solve this equation to get x = some function of t.

One simple case is a(x) = -x, which results in x(t) = e(sin(t+f)), where e and f are constants.
 
Last edited:
Thanks rgcldr!

great explanation and example!

fisico30
 
Hi rcgldr,

one question:

when you get v dv = f(x) dx, is v a function of t or of x, i.e. is v equal to v(t) or v(x)?

It looks like it would be a function of x, v(x), since 1/2 v^2 = g(x) + c results in v(x) = sqrt(2 (g(x) + c)).

I am confused because when we write v=dx/dt I always assume that v must be a function of time t, i.e. v(t).
When in your first step you write a(x) = dv/dt I tend to think that the v must be function of t since dv/dt is a derivative with respect to time.

So which one is correct? a(x)= dv(x)/dt or a(t)=dv(t)/dt. Acceleration is always the time derivative of the velocity vector but the velocity vector can be a function of any dependent variable: v(t), v(x), v(F), where F is force, etc...

Thanks,
fisico30
 
I guess my point is: if a function, like a, is defined as a time derivative of another function, dv/dt, does the differentiated function need to be a function if time?
 
fisico30 said:
when you get v dv = f(x) dx, is v a function of t or of x, i.e. is v equal to v(t) or v(x)? It looks like it would be a function of x, v(x), since 1/2 v^2 = g(x) + c results in v(x) = sqrt(2 (g(x) + c)).
At this point, it's just a relationship between v and x.

I am confused because when we write v=dx/dt I always assume that v must be a function of time t, i.e. v(t).
It is, but I was only able to take advantage of that in the last step where I find t as a function of x.

When in your first step you write a(x) = dv/dt I tend to think that the v must be function of t since dv/dt is a derivative with respect to time.
True, but I used chain rule to get rid of the dt and end up with v dv = f(x) dx.

So which one is correct? a(x)= dv(x)/dt or a(t)=dv(t)/dt.
Both are correct, but if acceleration is defined as a function of x, then it may not be possible to find an equation for acceleration as a function of time. In the simple example I gave, a(x) = -x, you will be able to find both a(x) and a(t). I ended up finding x(t) = e sin(t + f). You can take the derivative of this to find v(t), and the derivative of v(t) to find a(t), so a(x) = -x, and a(t) = -e sin(t+f). For other situations, you may not be able to solve for x(t), v(t), or a(t), in which case numerical integration will be required.
 
So it is mathematically legal and ok to write a derivative of a function even if
the independent variable a of the function and the differentiation variable b are not the same: f(a) and db to create df(a)/db...

I guess that is all the chain rule is about...
 

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