Constant acceleration kinematics doubt

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Discussion Overview

The discussion revolves around understanding the relationship between acceleration, distance, and velocity in the context of kinematics, particularly focusing on the implications of using an acceleration versus distance graph. Participants explore the mathematical and conceptual aspects of these relationships, including the use of calculus and the conditions under which certain kinematic equations apply.

Discussion Character

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

Main Points Raised

  • One participant suggests that the area under an acceleration versus distance graph is incorrectly equated to velocity squared, questioning the validity of this interpretation.
  • Another participant clarifies that to find velocity from acceleration, one must consider the area under an acceleration versus time graph instead.
  • There is a mention that the area under the acceleration versus distance graph has a physical meaning, although it is not clearly explained, and it is suggested that this may be complex for beginners in kinematics.
  • A participant introduces the idea that calculus can be used to derive relationships between acceleration and velocity, indicating that the area under the acceleration curve can yield results applicable to varying acceleration functions.
  • Further discussion includes how to transform the relationship between acceleration and distance into velocity or acceleration versus time graphs, emphasizing the importance of understanding the dependencies between these variables.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of the area under the acceleration versus distance graph, with some asserting it does not directly relate to velocity squared, while others suggest it has a meaningful interpretation. The discussion remains unresolved regarding the exact implications of these relationships and the appropriate methods for analysis.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about constant acceleration and the mathematical steps involved in transitioning between different forms of kinematic equations. The participants also highlight the complexity introduced by non-constant acceleration, which remains a point of contention.

zuppi
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Hi,
I hope it is a very simple mistake and easy to spot.
Suppose you start at rest so initial velocity is 0 and you accelerate constantly over a certain distance.
An acceleration vs. distance graph (not time) would be like a rectangle. The area under the graph would be A=as=(s/t2)*s = v2.
According to v2=u2+2as, so that v2=2as and not as. I can't work out if the math or the general idea is wrong.

Hopefully I was clear enough. Thanks for any help!
zuppi
 
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What you did was basically find [itex]\int a ds[/itex] which is not going to equal the velocity squared. Why should it? Just because the units are the same doesn't mean the actual quantities are the same.
 
To get the velocity from the acceleration, you have to find the area under the graph of acceleration against time, not acceleration against distance.

Actually, the area under the graph of acceleration against distance does mean something physical, but if you are just starting to study kinematics, you probably don't know enough physics yet to give a simple explanation of what it means.
 
AlephZero said:
Actually, the area under the graph of acceleration against distance does mean something physical, but if you are just starting to study kinematics, you probably don't know enough physics yet to give a simple explanation of what it means.

Shhh, don't blab the secret out like that.
 
Thanks!
How can I get any useful information out of an acceleration vs distance graph if the acceleration is not constant? The area is not v2 or 1/2 v2 is it?
 
Now it seems you want to do calculus! Good for you, this is more or less the question Newton asked himself. Formulas like v2=2as are to make it so you don't have to do calculus, but they require constant a. The calculus says that you can use a=v*dv/ds and the area as is more generally an integral that results in v2/2, if v starts out zero. What's interesting is that this will be the area under the a vs. s graph for any function a(s), not just constant a. But until you get calculus, you will only treat constant a, and then the area is rectangular, just as you said. The kinematic formula tells you how to connect that area to the resulting final v, but when you notice that v2 comes out twice the area under the a(s) curve for constant a, it turns out that is also true for any a(s), which is I think just what you were speculating.
 
Last edited:
Thats good so I can integrate a(s) to get half v2. How can I use calculus to transform that into a velocity or acceleration versus time graph so I can calculate the total time taken?
 
Ah, so you are taking physics at the calculus level. This kind of thing gets easier once you've seen it a few times. If you have a(s), and we know this = v*dv/ds for getting v(s), now you just need v(t). Sometimes it is easier to start with what you want to know, which here is what is going on with t, so then you are looking for t(v) rather than v(t), but you can see that it is basically the same thing. Here's how you use calculus to get t(v):
t = integral over dt = integral over ds of dt/ds = integral over ds of 1/v(s).
You see how I got that by basically saying dt = ds*dt/ds, which is just like multiplying and dividing by ds? The idea there is if s is your independent variable, it means you have a lot of information about how things depend on s. That means you want to convert your integrals into integrals over ds, so you don't want to do an integral like integral over dt of a(t), since t is not your independent variable here and you don't know anything about how things depend on t.
 
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