Integrating motion equation to derive displacement

  • #1
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##\frac{dx}{dt} = \frac{dx_i}{dt} + \frac{d^2x}{dt^2}t##
Multiplying dt on both sides and integrating we have
##\int_{x_f}^{x_i} dx = \int_{0}^{v_i t} dx_i + \int_{0}^{at} dvt##
so ##x_f - x_i = v_it + at^2##, which is not right

Where did I go wrong?

I understand that if we substitute a for ##\frac{d^2x}{dt^2}##, integrating atdt = 0.5at, but what if we derived the equation for displacement by multiplying by dt?
 

Answers and Replies

  • #2
##\frac{dx}{dt} = \frac{dx_i}{dt} + \frac{d^2x}{dt^2}t##
Multiplying dt on both sides and integrating we have
##\int_{x_f}^{x_i} dx = \int_{0}^{v_i t} dx_i + \int_{0}^{at} dvt##
so ##x_f - x_i = v_it + at^2##, which is not right

Where did I go wrong?

I understand that if we substitute a for ##\frac{d^2x}{dt^2}##, integrating atdt = 0.5at, but what if we derived the equation for displacement by multiplying by dt?
What is ##x_i##?
 
  • #3
What is ##x_i##?
##x_i## is Initial position. I swapped the ##x_i## and ##x_f## positions in the integral
 
  • #4
And does the initial position change as the object is in motion?
 
  • #5
And does the initial position change as the object is in motion?
No, the initial position is constant
 
  • #6
So what is ##dx_i## if ##x_i## is constant?
 
  • #7
No, the initial position is constant
If ##x_i## is constant, what are the meanings of ##\frac{dx_i}{dt} ## and ##dx_i## in your Post #1 equations?

It is not clear what question you are trying to answer. E.g. is this about an object with constant or variable acceleration? A complete and clear problem-statement is needed.
 
  • #8
So what is ##dx_i## if ##x_i## is constant?
Wow, you beat me by a fraction of a second. I avoided replying for about an hour in case you replied. But then gave way to temptation!
 
  • #9
Wow, you beat me by a fraction of a second. I avoided replying for about an hour in case you replied. But then gave way to temptation!
I appreciate the consideration. I was out walking the dog.

It is not clear what question you are trying to answer. E.g. is this about an object with constant or variable acceleration? A complete and clear problem-statement is needed.
I think @annamal started with ##v=v_i+at##, substituted ##v=\frac{dx}{dt}##, ##v_i=\frac{dx_i}{dt}## and ##a=\frac{d^2x}{dt^2}## and now wants to know how to solve this equation for ##x##.

To @annamal : It looks like you need a course in ordinary differential equations. For the time being, start with ##\frac{dv}{dt}=a## where a is constant. Integrate that to get the velocity as a function of time, ##v(t)##. Don't forget the integration constant. Then integrate once more ##\frac{dx}{dt}=v(t)## to find ##x(t)##. Again, don't forget the integration constant.
 
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  • #10
I appreciate the consideration. I was out walking the dog.


I think @annamal started with ##v=v_i+at##, substituted ##v=\frac{dx}{dt}##, ##v_i=\frac{dx_i}{dt}## and ##a=\frac{d^2x}{dt^2}## and now wants to know how to solve this equation for ##x##.

To @annamal : It looks like you need a course in ordinary differential equations. For the time being, start with ##\frac{dv}{dt}=a## where a is constant. Integrate that to get the velocity as a function of time, ##v(t)##. Don't forget the integration constant. Then integrate once more ##\frac{dx}{dt}=v(t)## to find ##x(t)##. Again, don't forget the integration constant.
I have taken differential equations already, so feel free to explain it to me in those terms as well

Yes, you're right in my intention, but I don't want to integrate in that way. I want to multiply dt throughout the equation and then integrate. so instead of saying ##\frac{dv}{dt}dt## = adt, we multiply dt so that adt = dv and then integrate. I am wondering why I can't derive the equation for position by multiplying dt throughout with a starting equation of ##\frac{dx}{dt} = \frac{dx_i}{dt} + \frac{d^2x}{dt^2}t##. Multiplying dt and integrating:

##\int_{x_i}^{x_f} dx = \int_{0}^{v_i t} dx_i + \int_{0}^{at} dvt##
 
  • #11
##\int_{x_i}^{x_f} dx = \int_{0}^{v_i t} dx_i + \int_{0}^{at} dvt##
This equation is nonsense. To begin with, if ##x_i## is the initial position, it is a constant which means that ##dx_i=0##. As ##dvt##, it is meaningless unless you mean ##d(vt)=vdt+tdv## in which case you must write that.
Now for what you want to do.
I am wondering why I can't derive the equation for position by multiplying dt throughout with a starting equation of ##\frac{dx}{dt} = \frac{dx_i}{dt} + \frac{d^2x}{dt^2}t##. Multiplying dt and integrating.
You can't because you are going around in a vicious circle. The equation
$$x=x_i+v_it+\frac{1}{2}at^2$$was the result of integrating twice the equation $$\frac{d^2x}{dt^2}=a=\mathbf{constant}.$$ You can't go back to the equation you derived and replace the constant ##a## with a function of time ## \dfrac{d^2 x}{dt^2}## and expect something sensible to emerge.
 
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  • #12
For those(*) helping with this thread, you might want to check the thread: https://www.physicsforums.com/threads/integrating-motion-equation-to-derive-displacement.1015857/
in the Classical Physics Forum (which is where this thread started before being moved).
* @kuruman, @Steve4Physics
 
  • #13
Your link take you back to this thread. It is self-referencing. Or maybe your intention was to post it in the other thread?
 
  • #14
Your link take you back to this thread. It is self-referencing. Or maybe your intention was to post it in the other thread?
I believe @SammyS very cleverly provided a self-referencing link to match the self-referencing "derivation" by @annamal.
 
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  • #17
To add to what has been said:$$v_i = v(t_i) \equiv v\rvert_{t=t_i} \equiv \frac{dx}{dt}\rvert_{t = t_i}$$In other words, ##v_i## is the velocity function of time evaluated at a specific time ##t_i##. Likewise ##x_i## is the position function of time evaluated at ##t_i##. It's not a function of ##t##, so ##\dfrac{dx_i}{dt}## is meaningless.
 

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