My possible misunderstanding on a freely falling object

Click For Summary

Discussion Overview

The discussion revolves around the application of kinematic equations to freely falling objects, specifically whether the equations can be applied to different points along the trajectory of a falling object. Participants explore the implications of using the equations for various points in time and space, and whether they yield consistent results.

Discussion Character

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

Main Points Raised

  • Some participants assert that the kinematic equations can be applied to any point along the trajectory of a falling object, with each point corresponding to a different time.
  • Others propose that using the equations for different points A and B, with their respective initial positions and velocities, leads to distinct parabolas unless A and B are the same point.
  • A participant questions whether the equations yield the same values for different points after a specified time, suggesting a need for rigorous proof.
  • Some participants discuss the distinction between parabolas in space versus those in spacetime, indicating a potential source of confusion in the application of the equations.
  • There is a suggestion to treat each axis separately to simplify the analysis of the motion.
  • One participant expresses uncertainty about the relationship between time and a parameter used to describe the parabola, indicating a need for further exploration.
  • Another participant points out that defining too many variables may lead to confusion regarding the initial conditions of points A and B.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether the kinematic equations can be universally applied to different points along the trajectory of a freely falling object. Multiple competing views remain regarding the interpretation of the equations and their application to distinct points in space and time.

Contextual Notes

Limitations include the potential confusion arising from the definitions of initial conditions for different points, the distinction between spatial and temporal representations of motion, and the assumptions made about the relationship between time and other parameters in the equations.

Anama Skout
Messages
53
Reaction score
13
Consider the famous kinematics equations $$x_f=x_i+v_i\cdot t+\frac12at^2$$ My question is: does this equation work for every point A & B along the parabola formed when dropping an object?
 
Physics news on Phys.org
Yes. Each point is represented by a different t. To make that clear, I would write it as:

$$x(t)=x_0+v_0 t+\frac{1}{2}a t^2$$
 
  • Like
Likes   Reactions: Anama Skout
DaleSpam said:
Yes. Each point is represented by a different t. To make that clear, I would write it as:

$$x(t)=x_0+v_0 t+\frac{1}{2}a t^2$$
Thanks for your answer. But I have something different in mind. Suppose that the point A has ##x_{A,0}## and ##v_{A,i}##, then the equation will have the form $$x_A(t)=x_{A,i}+v_{A,i}\cdot t+\frac12at^2$$ and for a point B which has ##x_{B,0}## and ##v_{B,i}## then the equation will have the form $$x_B(t)=x_{B,i}+v_{B,i}\cdot t+\frac12at^2$$ Will this yield the same values in that for instance if we use them to determine what will happen after ##t=5## as long as we know what ##x_{A,0}##, ##v_{A,i}##, ##x_{B,0}##, and ##v_{B,i}## are (and the time difference between the two)?
 
Anama Skout said:
Will this yield the same values in that for instance if we use them to determine what will happen after ##t=5## as long as we know what ##x_{A,0}##, ##v_{A,i}##, ##x_{B,0}##, and ##v_{B,i}## are (and the time difference between the two)?
Why don't you try it and see for yourself?
 
Doc Al said:
Why don't you try it and see for yourself?
I tried it with three points, always worked well (except the times when I made some mistakes -- of course), however I'm more interested into a rigorous proof.
 
Anama Skout said:
however I'm more interested into a rigorous proof.
Should be doable with a bit of algebra. Go for it!
 
I know it must be a simple thing I'm missing, but I can't figure it out, here's my try. Consider two points A & B such that ##x_{A,i}=R+x_{B,i}## and ##v_{A,i}\neq v_{B,i}## (for generality), then I should show that
  1. it implies that ##x_{A,f}=R+x_{B,f}##
  2. it implies that the final velocities won't change (how do I formulate that?)
I arrived at the following equations $$v_{A,f}-v_{B,f}=v_{A,i}-v_{B,i}\\x_{A,f}-x_{B,f}-R=t(v_{A,i}-v_{B,i})$$
And for that equality to happen we must have ##v_{A,i}-v_{B,i}=0## but this contradicts our assumption that ##v_{A,i}\neq v_{B,i}##, since clearly if -- for example -- you have an object falling onto the ground, if you take two distinct points in its trajectory, the velocity at each point won't be the same.

So what am I missing?

(here's a visualization of the situation)
 

Attachments

  • Snapshot.jpg
    Snapshot.jpg
    6.4 KB · Views: 505
Anama Skout said:
Thanks for your answer. But I have something different in mind. Suppose that the point A has ##x_{A,0}## and ##v_{A,i}##, then the equation will have the form $$x_A(t)=x_{A,i}+v_{A,i}\cdot t+\frac12at^2$$ and for a point B which has ##x_{B,0}## and ##v_{B,i}## then the equation will have the form $$x_B(t)=x_{B,i}+v_{B,i}\cdot t+\frac12at^2$$ Will this yield the same values in that for instance if we use them to determine what will happen after ##t=5## as long as we know what ##x_{A,0}##, ##v_{A,i}##, ##x_{B,0}##, and ##v_{B,i}## are (and the time difference between the two)?
The given form of the equation only works for ##x_0## and ##v_0## defined at ##t=0##. At ##t=0## the object is only at one point. If you use the same formula for a point which is on the parabola at a different time then you are going to get a different parabola which has that point at ##t=0##.

In other words, unless ##A=B## the equations that you have written represent two distinct parabolas. I.e. the first equation passes through ##A## at ##t=0## and the second equation passes through ##B## at ##t=0##, they are not the same parabola even if both parabolas pass through ##A## and ##B##.

Also, I am not sure if you are thinking about parabolas through space or parabolas in spacetime. The equation you have written is for 1D motion, so it is only a parabola in spacetime.
 
DaleSpam said:
The given form of the equation only works for ##x_0## and ##v_0## defined at ##t=0##. At ##t=0## the object is only at one point. If you use the same formula for a point which is on the parabola at a different time then you are going to get a different parabola which has that point at ##t=0##.

In other words, unless ##A=B## the equations that you have written represent two distinct parabolas. I.e. the first equation passes through ##A## at ##t=0## and the second equation passes through ##B## at ##t=0##, they are not the same parabola even if both parabolas pass through ##A## and ##B##.

Also, I am not sure if you are thinking about parabolas through space or parabolas in spacetime. The equation you have written is for 1D motion, so it is only a parabola in spacetime.

Ah, forgot about time, I should have added the following constraints ##t_B=T+t_A##, but again this doesn't yield much...
 
  • #10
So are you thinking of parabolas in space parametrized by time or are you thinking of parabolas in spacetime?
 
  • #11
DaleSpam said:
So are you thinking of parabolas in space parametrized by time or are you thinking of parabolas in spacetime?
I'm thinking of parabolas in space parametrized w.r.t time. (like the one I drawed)
 
Last edited:
  • #12
Why don't you treat each axis separately? I would think that would be simpler.
 
  • #13
Doc Al said:
Why don't you treat each axis separately? I would think that would be simpler.
I only treated the system w.r.t to a coordinate system in which the ##x##-axis is vertical.
 
  • #14
Anama Skout said:
I only treated the system w.r.t to a coordinate system in which the ##x##-axis is vertical.
Ah, so you are only talking about the vertical axis (as I first thought) despite the mention of parabolas. OK.
 
  • #15
Anama Skout said:
I'm thinking of parabolas in space parametrized w.r.t time. (like the one I drawed)
I am not quite sure why you want to put yourself through this, but OK. So a parabola in space can be defined by the parametric equations:
##x(\tau)=p \tau^2 + h##
##y(\tau)=2 p \tau + k##
##z(\tau)=0##
Where the vertex of the parabola is at ##(x,y,z)=(h,k,0)##, and ##p## indicates how flat the parabola is. The x direction is vertical, the y direction is horizontal along the arc of the parabola and the z direction is perpendicular to the parabola.

##\tau## is not time, it is a somewhat arbitrary parameter. To use this approach then you would need to solve for the relationship between ##\tau## and ##t##. That would involve some more free parameters which would allow you to have the same spatial parabola represented by the same equations in ##\tau## independently of when the object passes through any given points on the parabola.

I leave the details of figuring out the relationship between time and ##\tau## to you.
 
  • #16
DaleSpam said:
Yes. Each point is represented by a different t. To make that clear, I would write it as:

$$x(t)=x_0+v_0 t+\frac{1}{2}a t^2$$
How would this equation work for parabola? This is a straight line equation isn't it?
 
  • #17
Hamza Abbasi said:
How would this equation work for parabola? This is a straight line equation isn't it?
The motion is along a straight line. But expressed as a function of time, the equation describes a parabola.
 
  • #18
Anama Skout said:
Thanks for your answer. But I have something different in mind. Suppose that the point A has ##x_{A,0}## and ##v_{A,i}##, then the equation will have the form $$x_A(t)=x_{A,i}+v_{A,i}\cdot t+\frac12at^2$$ and for a point B which has ##x_{B,0}## and ##v_{B,i}## then the equation will have the form $$x_B(t)=x_{B,i}+v_{B,i}\cdot t+\frac12at^2$$ Will this yield the same values in that for instance if we use them to determine what will happen after ##t=5## as long as we know what ##x_{A,0}##, ##v_{A,i}##, ##x_{B,0}##, and ##v_{B,i}## are (and the time difference between the two)?
The confusion here is that you have defined too many variables. Point i or 0, is a chosen initial point on the trajectory. A and B are two other points on the same trajectory. So there is no separate initial position for A and a separate one for B.
 
  • #19
E
Doc Al said:
The motion is along a straight line. But expressed as a function of time, the equation describes a parabola.
Equation is of straight line but it explains parabola?? How come?
 
  • #20
Hamza Abbasi said:
Equation is of straight line but it explains parabola?? How come?
If you plot x as a function of time, it is not a straight line.
 
  • #21
Hamza Abbasi said:
How would this equation work for parabola? This is a straight line equation isn't it?
It is a straight line in space. It is a parabola in spacetime.
 
  • #22
DaleSpam said:
It is a straight line in space. It is a parabola in spacetime.
Wow! I didn't knew that :oldlove: , can you please post some pictorial representation?
 
  • #23
Hamza Abbasi said:
Wow! I didn't knew that :oldlove: , can you please post some pictorial representation?
You have the function. Plot it for yourself!
 
  • #24
Anama Skout said:
Thanks for your answer. But I have something different in mind. Suppose that the point A has ##x_{A,0}## and ##v_{A,i}##, then the equation will have the form $$x_A(t)=x_{A,i}+v_{A,i}\cdot t+\frac12at^2$$ and for a point B which has ##x_{B,0}## and ##v_{B,i}## then the equation will have the form $$x_B(t)=x_{B,i}+v_{B,i}\cdot t+\frac12at^2$$ Will this yield the same values in that for instance if we use them to determine what will happen after ##t=5## as long as we know what ##x_{A,0}##, ##v_{A,i}##, ##x_{B,0}##, and ##v_{B,i}## are (and the time difference between the two)?
If I understand you correctly, ##x_{B,i}## and ##v_{B,i}## are the position and velocity of the particle some time (say ##\Delta t##) after it passes through ##x_{A,i}##. So all you need to show is that the position given by the first equation at time ##t + \Delta t## is the same as the position given by the second equation at time ##t##. That's why I said it was just a bit of algebra.

Of course you'll need to express ##x_{B,i}## and ##v_{B,i}## in terms of ##x_{A,i}##, ##v_{A,i}##, and ##\Delta t##.
 
  • #25
It is not clear what you mean by your notation. You may be using it in a weird way.
For example, what is [itex]x_A[/itex]? If it is the position of point A, a point on the trajectory? It this is so, then it does not make sense to write [itex]x_A(t)[/itex]. The point is fixed, there is no time dependence for the position of that point.
Or A is some object moving along the trajectory and [itex]x_A(t)[/itex] is the position of this object.
Then B should be another object, starting from a different position? Is this what you mean?
You have two objects?
 
  • #26
Okay, sorry, it is all my fault for using a notation that I didn't properly explain. I'll use an example to illustrate what I want to show

A stone thrown from the top of a building is given an initial velocity of 20.0 m/s straight upward. The stone is launched 50.0 m above the ground, and the stone just misses the edge of the roof on its way down as shown in the figure below.
22q5A.png

In this example, I used the point A as the initial point. Now consider as if we're working with points B & C. All the values shown in the figure are relative to A. You can see that ##t_B=\rm{2.04 \;sec}## -- with that notation -- with respect to A, but it would be ##0\;\rm sec## with respect to B, or ##-2.04\;\rm sec## with respect to C.

Now what happens when the time passed from the initial time ##t=5\,\rm sec## ##\color{green}{\text{(with respect to A)}}##, i.e. what's the position & velocity at that time?

Well, we know that $$x_f=x_i+v_it+\frac12at^2,\tag{1}$$ we have that ##x_i=0{\rm\;sec},v_i=20.0\rm\;m/s## hence we get that $$\bbox[8pt,lightgreen,border:3px green solid]{\color{}{\large x_f=-22.5\rm\;m}}\tag{2}$$ Now, ##\color{blue}{\text{with respect to C}}##, we have that ##x_i={\rm\;0m},v_i=-20.0{\rm\;m/s},t=\big(5-4.08\big){\rm\;s}=0.92{\rm\;s}##, putting these values in ##(1)##, and sure enough: $$\bbox[8pt,skyblue,border:3px blue solid]{\color{}{\large x_f=-22.5\rm\;m}}\tag{3}$$ Now, ##\color{red}{\text{with respect to B}}## we have that ##x_i=0{\rm\;m},v_i=0{\rm\;m/s},t=\big(5-2.04\big){\rm\;m}=2.96{\rm\;m}##. Putting these things in ##(1)## yields $$\bbox[8pt,pink,border:3px red solid]{\color{}{\large x_f=-43\rm\;m}}\tag{4}$$ I assume these would lead us, under the correct transformation, to ##x_f## with respect to A.

But basically you got the idea, showing that no matter what points B & C we choose, it will always the same result, up to the change in the distance between them.
 
Last edited:
  • #27
Well, why use x when all your labels in the picture are y? But this is a minor point.
You did not make any mistake.
The position is -22.5 m in respect to A but -42.9 m in respect to B. Did you expect to get the same value? You are measuring (same) position from different origins. It will be unlikely to get the same value. If you look at the figure you can see that the distance from B to D is larger than from A to D.(or than C to D).
 
  • Like
Likes   Reactions: Anama Skout
  • #28
nasu said:
Well, why use x when all your labels in the picture are y? But this is a minor point.
You did not make any mistake.
The position is -22.5 m in respect to A but -42.9 m in respect to B. Did you expect to get the same value? You are measuring (same) position from different origins. It will be unlikely to get the same value. If you look at the figure you can see that the distance from B to D is larger than from A to D.(or than C to D).
Oups, another mistake, I wanted to say that we would get the same result between these points if we translate one to another. I'll edit the earlier post.
 
  • #29
I don't know what you mean by this "translate one to another". By changing the origin, the values of the coordinate will change and there is no mistake.
The positions will change but speed and acceleration won't change if you translate the origin to a different point along the same line.
 
  • Like
Likes   Reactions: Anama Skout
  • #30
nasu said:
I don't know what you mean by this "translate one to another". By changing the origin, the values of the coordinate will change and there is no mistake.
The positions will change but speed and acceleration won't change if you translate the origin to a different point along the same line.
In this case I translated A to B, the difference between the x-coordinate of the two is only 2.04 m, and doesn't help to get 22.5 m out of the 43 m, why?

Also, I agree that the change in the coordinate only amounts to a change in the origin, so there will be no differnece, okay. But why the speed won't change? I mean, conceptually, yes, it will be the same, but I'm looking for a rigorous derivation.
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 26 ·
Replies
26
Views
10K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 5 ·
Replies
5
Views
9K
  • · Replies 35 ·
2
Replies
35
Views
5K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 11 ·
Replies
11
Views
7K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K