Integrating motion equation to derive displacement

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Homework Help Overview

The discussion revolves around the integration of motion equations to derive displacement, specifically focusing on the relationship between velocity, acceleration, and position in the context of kinematics. Participants explore the implications of integrating equations involving derivatives of position with respect to time.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants examine the integration of motion equations, questioning the validity of certain steps and the definitions of variables such as initial position. There is a focus on whether the initial position changes during motion and the implications of treating certain variables as constants.

Discussion Status

The discussion is ongoing, with participants providing insights and questioning each other's reasoning. Some guidance has been offered regarding the integration process and the need for clarity in problem statements. Multiple interpretations of the equations and their components are being explored.

Contextual Notes

There are constraints regarding the clarity of the problem statement, as some participants express confusion over the definitions and roles of variables like ##x_i## and ##dx_i##. The discussion also touches on the distinction between constant and variable acceleration.

annamal
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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?
 
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annamal said:
##\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##?
 
kuruman said:
What is ##x_i##?
##x_i## is Initial position. I swapped the ##x_i## and ##x_f## positions in the integral
 
And does the initial position change as the object is in motion?
 
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kuruman said:
And does the initial position change as the object is in motion?
No, the initial position is constant
 
So what is ##dx_i## if ##x_i## is constant?
 
annamal said:
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.
 
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kuruman said:
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!
 
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Steve4Physics said:
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.

Steve4Physics said:
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
kuruman said:
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
annamal said:
##\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.
annamal said:
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
 
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  • #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?
 
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nasu said:
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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