Acceleration on a position vs. time graph can be obtained, by having the initial position and velocity of a moving object.

In this article, we want to show you how to find constant acceleration from a position-time graph with some solved problems.

*You can skip this introduction and refer to problems 6 and 7. *

## Types of Motion:

An object can move *at a constant speed* or have a *changing velocity*.

Suppose you are driving a car at a constant speed of $100\,{\rm km/h}$ along a straight line. What does mean by $100\,{\rm km/h}$?

The speed of $100\,{\rm km/h}$ indicates that you drive the first 100 km in the first hour, the next 100 km during the second hour, another 100 km for the third hour, and so on.

Once we plot these successive equal displacements as a function of time, we arrive at a straight line.

As you can see above, at equal time intervals (here, 1 second) every second the displacements $\Delta x_1$ and $\Delta x_2$ are equal.

In such a type of motion, during each equal time interval, displacements are equal. This kind of motion is called ** uniform motion** since, by definition of average acceleration, the object's acceleration is zero.

According to the definition of average velocity, $\bar{v}=\frac{x-x_0}{\Delta t}$, we can find the position of a moving object at each instant by rearranging it as below \[x=vt+x_0\] This is a linear equation with a position vs. time graph shown above.

Therefore, **a motion in which equal displacements occur during any successive equal-time intervals is known as uniform motion.**

Now, when the car has a **changing velocity**, and we plot the positions of each point that the car passes through it, we arrive at an

__, in contrast to a straight line in the previous case.__

**arbitrary curve**In the above, you can see explicitly that at each equal time intervals (here, $1\,{\rm s}$) the corresponding displacements are not equal i.e. $\Delta x_{BC}\ne \Delta x_{AB}$.

Therefore, the acceleration of such a motion is not zero.

In this case, the position of a moving object at any moment is given by the kinematics equation, $x=\frac 12 at^2 +v_0t+x_0$.

This equation tells us that for an accelerated motion, position varies with time in a quadratic form whose graph is shown above.

**Overall, a constant velocity (uniform) motion has a straight line position-versus-time graph, but a curve in the $x-t$ graph represents an accelerated motion.**

This curve for a constant acceleration has a simple form of quadratic.

## Direction of acceleration on a position-time graph

Acceleration is defined as a vector quantity in physics with both a direction and a magnitude. We can find both using a $x-t$ graph.

As mentioned above, the position of a uniform accelerating object varies with time as a quadratic function.

**A positive acceleration ($a>0$) yields a position-time graph opening upward**.

Similarly, **a negative acceleration ($a<0$) produces a position-time graph opening downward**. Both cases are shown in the figure below

Magnitude of acceleration on a position-time graph

It is a difficult task to find the magnitude of the acceleration vector for a moving object from its position-time graph.

If the object increases its speed at a constant rate, then its acceleration is a constant value during that time interval.

In such cases, the position vs. time graph has a quadratic curve in which we can simply find its acceleration by having initial position and velocity.

*In the following, we will try to learn this calculation by a couple of solved examples.*

**Example (1): The equation of position vs. time for a moving object, in SI units, is as $x=-t^2+6t-9$. Which of the following choices are correct?
(a) The object's acceleration is constant and its magnitude is $1\,{\rm m/s^2}$.
(b) The object's velocity at the initial time $t=0$ is to the negative $x$-axis.
(c) The object's initial position is on the negative side of the $x$-axis.**

**Solution**: we examine each choice separately.

(a) **This equation has a quadratic form so its acceleration is constant.** Comparing this equation with standard constant acceleration kinematic equation, $x=\frac 12 at^2+v_0t+x_0$, we will find its magnitude as \[\frac 12 a=-1 \Rightarrow \ a=-2\,{\rm m/s^2}\] So this choice is incorrect.

(b) "*Object's velocity at the initial time*'' means its initial velocity. Comparing the two equations below reveals that initial velocity is $v_0=+6\,{\rm m/s}$.\begin{gather*}x=\frac 12 at^2+v_0t+x_0 \\\\ x=-t^2+6t-9 \end{gather*} The positive sign indicates that the initial velocity is toward the positive $x$-axis. So, this choice is also incorrect.

(c) By setting $t=0$ in the position-time equation, its initial position is obtained. So, $x_0=-9\,{\rm m}$. Negative indicates that the object is on the negative side of the $x$-axis initially. Thus, this choice is correct.

**Example (2): The position vs. time graph of a moving object accelerates uniformly along the $x$ axis is plotted in the figure below. Find its acceleration, initial velocity, and position. **

**Solution**: __The concavity of the graph tells us about the sign of acceleration.__ Here, the graph opens upward (concave upward), so its acceleration is positive, $a>0$.

At the instant the motion is started $t=0$, the position of the object is a negative value. It means that, initially, the object starts its motion on the negative side of the $x$-axis.

Recall that the __slope of the position-time graph represents the object's velocity__. A tangent line at time $t=0$ has a negative slope because that makes an obtuse angle with the $+x$-axis. So, the initial velocity is negative, too.

Overall, this object starts its motion at a position behind the origin in the opposite direction of the $x$-axis as shown in the figure below.

In the next example, we will find the constant acceleration of a moving object using its position vs. time graph numerically.

**Example (3): the position of a moving object (along a straight positive line) as a function of time is given by the curve shown in the figure below. Find the acceleration of the object.**

**Solution**: First, collect all information that the plot gives us. At time $t=0$, the object is at position $x=-9\,{\rm m}$ and at time $t=3\,{\rm s}$ its position is zero, that is, it returns back to its starting position.

The graph opens upward, indicating a positive acceleration.

It is said that the motion has a constant acceleration, so its position versus time must be changed as a quadratic function which is determined by the kinematics equation $x=\frac 12 at^2+v_0t+x_0$.

In the above equation, $x_0$ is the position at time $t=0$ or the initial position. The graph shows us that, for this object, it is $x_0=-9\,{\rm m}$.

$v_0$ is also the initial velocity which is found by computing the slope of the position-time graph at time $t=0$.

As you can see, in this graph, the slope (in green) is parallel to the horizontal, makes an angle of zero, and consequently, its initial velocity is zero, $v_0=0$.

If we substitute these two finding into the standard kinematics equation $x=\frac 12 at^2+v_0t+x_0$, we get \[x=\frac 12 at^2-9\] The remaining quantity is the acceleration $a$.

There is another point that has not been used yet, $B=(x=0,t=3\,{\rm s})$. Substituting this point into the above equation, and solving for $a$ we get \begin{align*} x&=\frac 12 at^2-9\\\\0&=\frac 12 (a)(3)^2-9\\\\\Rightarrow a&=2\quad {\rm m/s^2}\end{align*} Therefor, the object's acceleration is $2\,{\rm m/s^2}$.

**Example (4): A car starts at rest and accelerates at a constant rate in a straight line. Its position-versus-time graph is shown in the figure below. Find the car's acceleration?**

**Solution**: This is another example problem that shows you how to find acceleration from a position vs. time graph.

Like previous example, locate two points on the graph with the given information. $A(x=-8\,{\rm m},t=0)$ and $B(x=0,t=2\,{\rm s})$. Using these two points and applying the kinematics equation $x=\frac 12 at^2+v_0t+x_0$, one can find the car's acceleration.

Putting point $A$ into the above equation, gives us \begin{align*} x&=\frac 12 at^2+v_0t+x_0\\\\-8&=\frac 12 a(0)^2+v_0(0)+x_0\\\\\Rightarrow \quad x_0&=-8\,{\rm m}\end{align*} It is said in the question that the car starts its motion from rest, so its initial velocity is zero, $v_0=0$. Now, substituting the second point $B$ into the standard equation, and solving for $a$, get \begin{align*}x&=\frac 12 at^2+v_0t+x_0\\\\0&=\frac 12 a(2)^2+0-8\\\\ 0&=2a-8\\\\\Rightarrow a&=4\quad {\rm m/s^2}\end{align*} So with the help of two points on the position vs. time graph, we were able to find the acceleration of the object.

In the next example, acceleration on a position-time graph gets in the case of having an initial velocity, $v_0\neq0$.

**Example (6): The position vs. time graph of a moving object along the positive $x$-axis is as follows. Find the object's acceleration.**

**Solution**: As always, to find the constant acceleration of a moving object from its position-versus-time graph, one should locate two points on the graph and substitute them into the standard kinematics equation $x=\frac 12 at^2+v_0t+x_0$.

Here, initial point has coordinate $A(x=18\,{\rm m},t=0)$ from which we can find the initial position, $x_0=18\,{\rm m}$.

The other point is $B(x=0,t=6\,{\rm s})$. Given the initial position, substitute the point B into the standard kinematics equation, we have \begin{gather*} x=\frac 12 at^2+v_0t+x_0\\\\0=\frac 12 a(6)^2+v_0 (6)+18 \\\\ \Rightarrow \boxed{18a+6v_0+18=0} \end{gather*} As you can see, we have one equation with two unknowns. We need an additional equation to be able to find the unknowns.

In the previous examples, the position-time graph had a zero slope and thus get a zero initial velocity.

Of the graph, we see that the slope at time $t=0$ is not zero so the object does not start from rest.

But how to find another equation?

To find that equation, we pay attention to an important note below:

The tangent line at point $B$ is horizontal so velocity at that time is zero, according to the equivalence of slope and velocity on a $x-t$ graph.

Substituting this extra information into another kinematics equation, $v=v_0+at$, we can find the initial velocity. \begin{gather*} v=v_0+at\\0=v_0+a(6)\\ \Rightarrow \boxed{6a+v_0=0} \end{gather*} Solving the above equation for $v_0$, we get $v_0=-6a$.

Now, substitute it into the first equation $18a+6v_0+18=0$ and solve for the unknown acceleration \begin{gather*} 18a+6v_0+18=0\\ 18a+6(-6a)+18=0\\ \Rightarrow a=1\quad {\rm m/s^2}\end{gather*} If we put this value into $v_0=-6a$, the initial velocity is also found.

Consequently, the car starts its motion toward the negative $x$ axis with an initial velocity of 6 m/s and increases its speed at a constant rate of $1\,{\rm m/s^2}$.

**Example (7): The position vs. time graph of a moving object along a straight line is a parabola as below. Find the equation of the object's velocity as a function of time? **

**Solution**:

Physical interpretation of graph: This object starts its motion at some initial velocity (because the slope at time $t=0$ makes an angle with horizontal) and decreases its speed at a constant rate (i.e. $a<0$ as can be seen from the concavity downward of the curve) until reaches point B where its velocity gets zero, changes its direction, and returns to the starting point in the opposite direction.

As you guess, this is exactly a description for motion that appears in a free-fall. In addition, such a graph appears also in the projectile motion problems.

As said, the curve of the position-time graph is a parabola that has a quadratic form. So, the object has a constant acceleration.

On the other side, the curve opens downward, so the acceleration is negative $a<0$.

In this curve, the coordinate of three points are given, $A(x=0,t=0)$, $B(x=8\,{\rm m},t=2\,{\rm s})$, and $C(x=0\,{\rm m}, t=4\,{\rm s})$.

The velocity of an object with a constant acceleration changes with time as $v=v_0+at$. Thus, we must find its initial velocity as well as acceleration.

To find the unknowns, it is better to apply kinematics equations between any two given points. Between points A and B, displacement is computed as \[\Delta x=x_B-x_A=8-0=8\quad{\rm m}\] Using kinematics equation, $v^2-v_0^2=2a\Delta x$, for these two points, we have \begin{gather*} v_B^2-v_A^2=2a\Delta x\\\\0-v_0^2=2(a)(8)\\\\\Rightarrow\quad \boxed{v_0^2=-16a}\end{gather*} where we used this note that velocity at point B is zero because the slope of the tangent line at that point is horizontal.

Now, we choose points A and C, compute their displacement, and apply the kinematics equation $x-x_0=\frac 12 at^2+v_0t$ \[\Delta x=x_C-x_A=0-0=0\] As expected since the objects returns to its starting point. \begin{gather*} \Delta x=\frac 12 at^2+v_0t\\\\0=\frac 12 (a)(4)^2+v_0(4)\\\\ \Rightarrow \quad \boxed{8a+4v_0=0} \end{gather*} Until now, we have two equations with two unknowns which is completely solvable.

The second equation, $8a+4v_0=0$, gives us $v_0=-2a$. Now, substitute it into the first equation \begin{gather*} v_0^2=-16a\\\\ (-2a)^2=-16a\\\\4a^2=-16a\\\\ \rightarrow\quad 4a(a+4)=0\end{gather*} Solving this equation for $a$, we get two solutions $a=0$, and $a=-4\,{\rm m/s^2}$.

The zero acceleration $a=0$ is not plausible, since it represents a constant velocity motion whose position-time graph is a straight line but in this problem, we have a curve.

Therefore, the acceptable acceleration is $a=-4\,{\rm m/s^2}$. By substituting this into either first ($v_0^2=-16a$) or second equation ($8a+4v_0$), and solving for $v_0$, we will get the initial velocity, \begin{gather*} 8a+4v_0=0 \\ \rightarrow (8)(-4)+4v_0=0\\ \Rightarrow v_0=8\,{\rm m/s}\end{gather*} As expected, since the tangent line at time $t=0$ has a positive slope.

Substituting these known values into the kinematics equation $v=v_0+at$, we will obtain the object's velocity as a function of time. \[v=8-4t\] This equation gives the variation of velocity as a function of time. When this equation is plotted, a velocity-time graph is obtained.

## Summary:

In this article, we found out how to compute the object's constant acceleration using a position-time graph.

Having the initial velocity $v_0$, calculate the displacement $\Delta x$ between two known points on the graph. Next, use the kinematics equation $\Delta x=\frac 12 at^2+v_0t$ and solve for the unknown acceleration $a$.

If the object has an initial velocity, then we need at least three points on the graph with known position and time coordinates.

In this case, the kinematics equation $v^2-v_0^2=2a\Delta x$ is also used.

**Author**: Dr. Ali Nemati

**Page Published**: 8-13-2021