How to interpret the equation of position with constant acceleration?

In summary, the equation x = x0 + v0 * t + 1/2 * constant acceleration * t^2 describes the position of a body at time t, where x0 is the initial position, v0 is the initial velocity, and the third term comes from integrating the acceleration function. This term represents the average speed over small intervals of time, and when added over all intervals, it gives the total displacement. This can be visualized as the area under a velocity vs. time graph.
  • #1
Matt2411
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x = x0 + v0 * t + 1/2 * constant acceleration * t^2

So this is supposed to be very very simple physics, but I still feel like there's a part of this equation I don't fully understand. The first term is the initial position of the body at t=0. The second term is the initial velocity at t=0, multiplied by the time elapsed since then. So far so good. Now, it's the third term I have trouble interpreting. I know it comes from integrating the acceleration function, but why exactly is it so?

I tried to reason it the following way: Let's assume a=2 m/s^2, and for the sake of simplicity make both the initial position and velocity zero. Ok, so if I want to know the position of this body at t=1, then given that constant acceleration, velocity at t=1 will be 2 m/s. So the body should have had a displacement of 2 metres, right?

But if I plug in the values in the formula, I'd get x = 1/2 * 2 m/s^2 * 1 s^2 = 1 metre. Why is this the case?

I know it must be pretty stupid, but I can't figure out what's wrong with my reasoning.
Thanks in advance!
 
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  • #2
Matt2411 said:
Ok, so if I want to know the position of this body at t=1, then given that constant acceleration, velocity at t=1 will be 2 m/s.
Right.

Matt2411 said:
So the body should have had a displacement of 2 metres, right?
Wrong. The velocity at t = 1 would be 2 m/s, but it starts out with v = 0. So the average speed over that first second is only 1 m/s.
 
  • #3
Doc Al said:
Wrong. The velocity at t = 1 would be 2 m/s, but it starts out with v = 0. So the average speed over that first second is only 1 m/s.

I see. But what happens when t=2, for example? Because then the velocity at time 2 would be 4 m/s (the average over those two seconds will be 2 m/s), while the total displacement is 8 metres.
 
  • #4
Matt2411 said:
x = x0 + v0 * t + 1/2 * constant acceleration * t^2

So this is supposed to be very very simple physics, but I still feel like there's a part of this equation I don't fully understand. The first term is the initial position of the body at t=0. The second term is the initial velocity at t=0, multiplied by the time elapsed since then. So far so good. Now, it's the third term I have trouble interpreting. I know it comes from integrating the acceleration function, but why exactly is it so?

I tried to reason it the following way: Let's assume a=2 m/s^2, and for the sake of simplicity make both the initial position and velocity zero. Ok, so if I want to know the position of this body at t=1, then given that constant acceleration, velocity at t=1 will be 2 m/s. So the body should have had a displacement of 2 metres, right?

But if I plug in the values in the formula, I'd get x = 1/2 * 2 m/s^2 * 1 s^2 = 1 metre. Why is this the case?

I know it must be pretty stupid, but I can't figure out what's wrong with my reasoning.
Thanks in advance!
Acceleration is change of velocity with respect to time. In case of constant acceleration ##a##, it is simply ##a = \frac{ v_{final}-v_{initial}}{t_{final}-t_{initial}} \Rightarrow v_{final} =v_{initial} + a (t_{final}-t_{initial})##. If ##v_{initial} =0, t_{initial} = 0## and ##t_{final} = t##, then ##v_{final} = at##. But calculation displacement is a challenge here. Because here velocity is not constant. It varies with time (##v=at##). So you cannot write that displacement=##v_{final}t = at^2## or something like this. To counter this problem you have to assume that within every sufficiently small interval of time ##\Delta t##, the velocity remains constant. So within an interval ##\Delta t## displacement will be ##v\Delta t = at\Delta t##. Now if you add all the displacements at all intervals you will get total displacement which is ##\Sigma at \Delta t##. This is nothing but integration and the result is ##\frac{1}{2} at^2##.
 
  • #5
For constant acceleration, v = v0 + a t, and the average velocity at time t is ( (v0) + (v0 + a t) ) / 2 = v0 + 1/2 a t. Then the distance traveled is v0 t + 1/a 2 t^2 .
 
  • #6
Matt2411 said:
x = x0 + v0 * t + 1/2 * constant acceleration * t^2

So this is supposed to be very very simple physics, but I still feel like there's a part of this equation I don't fully understand. The first term is the initial position of the body at t=0. The second term is the initial velocity at t=0, multiplied by the time elapsed since then. So far so good. Now, it's the third term I have trouble interpreting. I know it comes from integrating the acceleration function, but why exactly is it so?

I tried to reason it the following way: Let's assume a=2 m/s^2, and for the sake of simplicity make both the initial position and velocity zero. Ok, so if I want to know the position of this body at t=1, then given that constant acceleration, velocity at t=1 will be 2 m/s. So the body should have had a displacement of 2 metres, right?

But if I plug in the values in the formula, I'd get x = 1/2 * 2 m/s^2 * 1 s^2 = 1 metre. Why is this the case?

I know it must be pretty stupid, but I can't figure out what's wrong with my reasoning.
Thanks in advance!

If you plot a velocity vs. time graph you get a straight line with slope ##a##, the acceleration. The distance moved from times ##0## to ##t## is the area under the ##v## vs. ##t## graph between times ##0## and ##t## (do you see why?) So, the distance traveled between times ##0## and ##t## is the area of a triangle with base ##t## and height ##at##.
 
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  • #7
Matt2411 said:
I see. But what happens when t=2, for example? Because then the velocity at time 2 would be 4 m/s (the average over those two seconds will be 2 m/s), while the total displacement is 8 metres.
I think you forgot the factor if ½ .

(½)(2)(22) = ½⋅2⋅4 = 4, not 8 .
 
  • #8
Matt2411 said:
I see. But what happens when t=2, for example? Because then the velocity at time 2 would be 4 m/s (the average over those two seconds will be 2 m/s), while the total displacement is 8 metres.
At t = 2 the velocity will be 4 m/s. For those first 2 seconds the velocity went from zero to 4, for an average speed of 2 m/s. So the distance traveled would be 4 m, not 8.
 
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  • #9
Ray Vickson said:
If you plot a velocity vs. time graph you get a straight line with slope ##a##, the acceleration. The distance moved from times ##0## to ##t## is the area under the ##v## vs. ##t## graph between times ##0## and ##t## (do you see why?) So, the distance traveled between times ##0## and ##t## is the area of a triangle with base ##t## and height ##at##.

I think this is what I was looking for. So the term ##\frac{1}{2} at^2## is really the area of a triangle given by the change in velocity with respect to the initial velocity.

Relating it to Doc Al's answer above (please correct me if I'm wrong), another way to look at it would be as the area of half the rectangle given by base ##t## and height ##at## (which would be the average velocity over that time interval, times the interval). Right?

SammyS said:
I think you forgot the factor if ½ .

(½)(2)(22) = ½⋅2⋅4 = 4, not 8 .

Doc Al said:
At t = 2 the velocity will be 4 m/s. For those first 2 seconds the velocity went from zero to 4, for an average speed of 2 m/s. So the distance traveled would be 4 m, not 8.

Right, my bad. It's just I was trying to make sense of that 1/2 factor. Though I think I got it now with Ray's answer.

Thanks to all of you guys!
 
  • #10
Matt2411 said:
Relating it to Doc Al's answer above (please correct me if I'm wrong), another way to look at it would be as the area of half the rectangle given by base ##t## and height ##at## (which would be the average velocity over that time interval, times the interval). Right?
Right. And that half rectangle is the triangle that Ray was talking about.
 
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  • #11
Doc Al said:
Right. And that half rectangle is the triangle that Ray was talking about.

Exactly. Thanks for the help, I really appreciate it :smile:
 
  • #12
Since a picture is worth a thousand words.

yP9R4ez.png
 

1. What is the equation of position with constant acceleration?

The equation of position with constant acceleration is given by x = x0 + v0t + (1/2)at2, where x is the position at time t, x0 is the initial position, v0 is the initial velocity, a is the constant acceleration, and t is the time elapsed.

2. How do I interpret the equation of position with constant acceleration?

The equation of position with constant acceleration describes the position of an object at any given time t, given its initial position, initial velocity, and constant acceleration. It can be used to calculate the position of an object at any point in time, as well as to determine the distance traveled by the object.

3. What do the different variables in the equation represent?

x represents the position of the object at any given time t, x0 represents the initial position of the object, v0 represents the initial velocity of the object, a represents the constant acceleration of the object, and t represents the time elapsed.

4. How does constant acceleration affect the position of an object?

Constant acceleration causes the object to change its velocity by the same amount every second. This results in the object's position changing at a constant rate over time. The greater the acceleration, the faster the position of the object changes.

5. How can the equation of position with constant acceleration be applied in real-life situations?

The equation of position with constant acceleration can be applied in various scenarios, such as calculating the position of a falling object due to gravity, determining the position of a car accelerating or decelerating at a constant rate, or predicting the position of a projectile launched at a certain angle with a constant acceleration due to air resistance.

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