What is the Antiderivative of Position in Calculus?

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Discussion Overview

The discussion revolves around the concept of the antiderivative of position in calculus, specifically exploring what physical quantity, if any, this antiderivative represents. Participants engage in a technical examination of the implications of integrating position with respect to time, considering both theoretical and practical aspects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that the antiderivative of position, when integrated with respect to time, results in a quantity with units of length times time (m·s).
  • Others question whether there is a physical quantity that corresponds to these units, expressing uncertainty about its practical application.
  • A participant references line integrals and suggests that the integration of a position function over a curve might relate to the discussion, though others clarify that this is not the same context as the antiderivative of position.
  • There is a debate about whether the integral of position has a specific physical meaning, with some asserting that no commonly defined physical quantity exists for the resulting units.
  • One participant humorously compares the integration of position to nonsensical operations, emphasizing the need for meaningful interpretations in physics.

Areas of Agreement / Disagreement

Participants generally agree that the position function can be integrated, but there is no consensus on whether the resulting integral has a specific physical meaning. Multiple competing views remain regarding the interpretation of the units produced by this integration.

Contextual Notes

Participants express uncertainty about the implications of integrating position, particularly regarding the physical significance of the resulting units. There are also references to different mathematical contexts, such as line integrals, which may not directly apply to the current discussion.

Who May Find This Useful

This discussion may be of interest to students and educators in mathematics and physics, particularly those exploring the concepts of integration and physical interpretations of mathematical results.

JimbozGrapes
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Well sitting in math class today learning about antiderivatives we talked about the following

Accelerations antiderivative is velocity

and,

velocities antiderivative is position.

So I asked my teacher what the antiderivative of a position would be then, and he did not know.

So if someone could tell me what he antiderivative of a position would represent that would be a massive releif to my curiosity.

Thanks.
 
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Integrating the position function with respect to time would give you a quantity with units m s (length*time). Do you know of any physical quantity with those units? I don't.
 
well i have read this in line integrals that to integrate a continuous function f(x,y,z) which is here position function of an object over curve c integratef(g(t),h(t),k(t))lv(t)ldt where v(t)=dr/dt and coordinates x,y,z are functions of time i guess it has something to do this with this type of problem
 
Line integrals are something different. Seeing as the examples he listed were [itex]\int a(t)dt=v(t), \int v(t)dt=x(t)[/itex] it stands to reason he meant [itex]\int x(t)dt=X(t)[/itex]. This is of course not a line integral.
 
if position is integrated with respect to time it must be position function and its coordinates can be function of time also.Is it not so?
 
I am not quite sure what you mean with that, could you elaborate and perhaps give a concrete example?
 
suppose position function is f(x,y,z) of a particle where x,y,z are functions of time t i.e x=h(t) y=g(t) and z=k(t) then it can be integrated i think so
 
Of course it can. The question is whether or not there is a useful application for the integral of the position. I cannot think of one, that doesn't mean there isn't one of course. But your example just extends it to three dimensions which doesn't really change the physical interpretation.
 
Yes, no one is disputing that the position function can be integrated. What is in dispute is the idea that its integral must have some specific physical meaning. As Cyosis said in the first response to your post, if the position function is integrated with respect to time, then the result must have units of "length times time" or "meters times seconds". There is not regularly defined physics quantity that even has those units!
 
  • #10
Units:
Acceleration has the units of length /time^2. Taking the antiderivative of the acceleration causes you to multiply the acceleration units by time. So you end up with length/time which are the units of velocity. Taking the antiderivative of velocity, multiply by time again, to get units of length, which is ...um..length or distance. If you take the antiderivative of distance, you have to multiply by seconds again to get units of
length*time. Can you think of any physical measurement that you can do that gets you units of length*time?

You can certainly take antiderivatives of a function all day long if you want. Nothing is preventing you. The question though, is does that answer have any physical meaning? I could take cats and divide by the color red. Does that have any physical meaning? (I hope not :)
 
  • #11
Bah...beaten to the punch.
 
  • #12
thanks a lot for the responses everyone, so the antiderivative of a position would give the units length*time is what i gathered. so something like m*s, which is kind of interesting weather it has practical physical use or not haha. Ill have to run that by my teacher and hopefully get a bonus mark or two :) .
 
  • #13
Not a slap on the ears? A very patient teacher!:smile:
 

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