Deriving constant acceleration equations

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Discussion Overview

The discussion revolves around the derivation of equations for constant acceleration in physics, specifically addressing the integration of velocity and its relationship to acceleration. Participants explore the mathematical steps involved and seek clarification on the reasoning behind these derivations.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Homework-related

Main Points Raised

  • One participant expresses confusion about why integrating velocity leads to equations for constant acceleration, questioning the logic behind this process.
  • Another participant explains that starting from the definition of acceleration as the derivative of velocity allows for integration, leading to the equation v = at + v_0, where a is constant.
  • A different participant reiterates that the integration of v = dx/dt is necessary to derive kinematic equations, emphasizing that the integration process is valid only under the assumption of constant acceleration.
  • Further clarification is provided on how integrating the expression for velocity results in the position equation x = x_0 + v_0t + (1/2)at^2, with constants determined by initial conditions.
  • Some participants acknowledge that the derivation can be complex and express appreciation for clearer explanations that help them understand the concepts better.

Areas of Agreement / Disagreement

Participants generally agree on the mathematical steps involved in deriving the equations, but there is ongoing uncertainty about the conceptual understanding of why these steps are necessary and how they relate to constant acceleration.

Contextual Notes

The discussion highlights the dependence on the assumption of constant acceleration for the integration process to yield valid kinematic equations. Some participants express that their understanding is contingent on the clarity of the derivation steps.

Who May Find This Useful

This discussion may be useful for students struggling with calculus and physics concepts related to motion, particularly those seeking to understand the derivation of kinematic equations under constant acceleration.

Opus_723
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Tired and not understanding Calculus.

So, velocity equals dx/dt
and acceleration is dv/dt

But to derive the constant acceleration equations, my professor took the integral of vdt = dx, which we got from v = dx/dt.

I follow all of the math that comes after that, but I don't understand why this integral produces equations for constant acceleration. Why are we taking the integral of velocity if acceleration is the derivative of velocity, and why does this only work for constant acceleration?

Thanks.
 
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While I'm not quite sure of the desired equations, what you could be aiming at is like the following:
Let a = dv/dt be the constant acceleration.
Then integral( a dt) = integral( dv ) for suitable integral limits.
Since a is constant it slips through the integral and
a integral( dt ) = integral( dv )
For an initial value problem which specifies the velocity, v_0 at time t_0, one can solve this as
a (t - t_0) = v - v_0 => v = v_0 + a(t - t_0). Now suppose you'd like to get x into the act,
v = dx/dt
So,
dx/dt = v_0 + a(t - t_0)
Taking integrals with suitable limits,
integral( dx ) = integral( v_0 dt ) + a ( integral( t dt ) - t_0 integral( dt ) )
Taking x = x_0 at t = t_0
x - x_0 = v_0 (t - t_0) + a[ (t^2/2 - t_0^2/2) - t_0 (t - t_0) ]
=> x - x_0 = (t - t_0)[v_0 + a (t - t_0)/2]
And I hope I haven't messed up the algebra.

Is this the kind of thing you were looking for?
 
Opus_723 said:
Tired and not understanding Calculus.

So, velocity equals dx/dt
and acceleration is dv/dt

But to derive the constant acceleration equations, my professor took the integral of vdt = dx, which we got from v = dx/dt.

I follow all of the math that comes after that, but I don't understand why this integral produces equations for constant acceleration. Why are we taking the integral of velocity if acceleration is the derivative of velocity, and why does this only work for constant acceleration?

Thanks.
Just v= dx/dt can't "produce equations for constant acceleration" because that equation alone says nothing about constant acceleration. You can start from "acceleration= dv/dt" and write dv= adt where a is that constant acceleration. Since a is constant that's easy to integrate and gives [itex]v= at+ v_0[/itex]. NOW we can use v= dx/dt to write [itex]dx/dt= at+ v_0[/itex] so that dx= (at+v_0)dt and integrate both sides of that to get [itex]x= (a/2)t^2+ v_0t+ x_0[/itex]. Is that what your professor did?
 
Yes, sorry, I should have been more clear. My professor substituted v0+at for v to get (v0+at)dt = dx.

So, I see that any integration that results from this would have a as a constant, simply because a must be a constant in order to get through the integration. But I don't understand why we integrate this to get a kinematic equation. Simplified, this is basically v = dx/dt. Why do we integrate this to get kinematic equations? I don't understand the first logical leap here.
 
[tex]a(t) = a = \textrm{const.}[/tex]

By definition:

[tex]v(t) = \int a(t)\,dt[/tex]

[tex]= a \int dt = at + C_1[/tex]

To solve for C1, consider t = 0:

[tex]v(0) = v_0 = a*0 + C_1[/tex]

Hence C1 = v(0) and therefore:

[tex]v(t) = v_0 + at[/tex]

Now, by definition

[tex]x(t) = \int v(t)\,dt[/tex]

[tex]= \int (v_0 + at)dt[/tex]

[tex]= v_0t + \frac{1}{2}at^2 + C_2[/tex]

Consider t = 0:

[tex]x(0) = x_0 = C_2[/tex]

Therefore:

[tex]x(t) = x_0 + v_0t + \frac{1}{2}at^2[/tex]

Now, can you explain clearly what specifically about this derivation you don't understand?
 
Opus_723 said:
Yes, sorry, I should have been more clear. My professor substituted v0+at for v to get (v0+at)dt = dx.

So, I see that any integration that results from this would have a as a constant, simply because a must be a constant in order to get through the integration. But I don't understand why we integrate this to get a kinematic equation. Simplified, this is basically v = dx/dt. Why do we integrate this to get kinematic equations? I don't understand the first logical leap here.

A kinematic equation describes position in terms of elapsed time. The integral gives you the position,x, in terms of elapsed time,t.
 
cepheid said:
Now, can you explain clearly what specifically about this derivation you don't understand?

Noting. That was perfect, thank you. I don't know why, but I was just totally spacing out and needed it laid out in front of me. I think you made it clearer what was going on than my professor did. He wrote it out different at the start, but now I see it means the same thing, only this was more intuitive for me. Thanks a lot.
 
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