Looking outside the window of a moving train means seeing that another stationary train appears to be moving backward. How does a stationary train appear to move? Behind it lies a crucial concept of Relative Motion, which will help us explain why objects move differently in different frames. Suppose you are driving a car and you overtake the other car from behind. What happens is that the driver from the car behind you sees the car coming in the backward direction and eventually goes back. However, the person standing on the ground doesn’t see it as the car moving backward, although the driver behind sees it that way.
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In this article, we will cover the concept of relative velocity This concept falls under the broader category of kinematics which is a crucial chapter in Class 11 Physics.
The rate of change in the position of one object concerning another object with time is defined as the Relative Velocity of one object with another.
Mathematically, relative velocity can be represented as:
Relative velocity of object A concerning object B.
$ \vec{V}_{A B}=\vec{V}_A-\vec{V}_B$
Also read -
1. When Two Objects Move in the Same Direction:
$$
V_{\text {relative }}=V_{\mathbf{1}}-V_2
$$
Where:
2. When Two Objects Move in Opposite Directions:
$$
V_{\text {relative }}=V_{\mathbf{1}}+V_2
$$
Where:
3. For Two-Dimensional Motion (Vector Form):
If the velocities of two objects are given as vectors $\vec{V}_1$ and $\vec{V}_2$, the relative velocity is calculated as:
$$
\vec{V}_{\text {relative }}=\vec{V}_1-\vec{V}_2
$$
Here, subtraction is done using vector operations, accounting for both magnitude and direction.
Let's start with some important case
$ \begin{aligned}
& \overrightarrow{V_A}=\text { Velocity of object } A . \\
& \overrightarrow{V_B}=\text { Velocity of object } B \text {. }
\end{aligned}$
Then, the relative velocity of A w.r.t B is:
$
\vec{V}_{A B}=\vec{V}_A-\vec{V}_B
$
$\vec{V}_{A B}, \vec{V}_A, \vec{V}_B$ all are in the same direction. (If $\vec{V}_A>\vec{V}_{B \text { ) }}$
And Relative velocity of B w.r.t A is
$\begin{aligned}
\vec{V}_{B A} & =\vec{V}_B-\vec{V}_A \\
\& \vec{V}_{A B} & =-\vec{V}_{B A}
\end{aligned}$
The relative velocity of A concerning B is.
$\begin{aligned}
& \vec{V}_{A B}=\vec{V}_A-\vec{V}_B \\
& V_{A B}=V_A+V_B
\end{aligned}$
Relative velocity of a body, A with respected body B
$
\begin{aligned}
V_{A B} & =\sqrt{V_A^2+V_B^2+2 V_A V_B \cos (180-\theta)} \\
& =\sqrt{V_A^2+V_B^2-2 V_A V_B \cos (\theta)}
\end{aligned}
$
Where,
$V_A=$ velocity of $A$
$V_B=$ velocity of $B$
$\theta=$ angle between $A$ and $B$
$ \begin{aligned}
& \tan \beta=\frac{V_B \sin (180-\theta)}{V_A+V_B \cos (180-\theta)} \\
& =\frac{V_B \cdot \sin \theta}{V_A-V_B \cos \theta}
\end{aligned}$
Relative Velocity of A concerning B is:
$V_{A B}=\sqrt{V_A^2+V_B^2}$
Example 1: A train is moving at 50 km/h and a man is running at 20 km/h in a direction opposite to the direction of the train. The relative velocity of the train (in km/h ) concerning man is
1) 70
2)30
3)60
4)40
Solution:
When A & B are moving along with straight line in the opposite direction.
$
\begin{aligned}
& \vec{V}_A=\text { Velocity of object } \mathrm{A} . \\
& \vec{V}_B=\text { Velocity of object } \mathrm{B} \text {. }
\end{aligned}
$
The relative velocity of $A$ concerning $B$ is.
$
\vec{V}_{A B}=\vec{V}_A-\left(-\vec{V}_B\right)
$
$-\vec{V}_B$ is because of the opposite direction.
$
\vec{V}_{A B}=\vec{V}_A+\left(\vec{V}_B\right)
$
As per question
$
\overrightarrow{V_R}=V_T+V_M
$
= ( 50 + 20 ) km/h
= 70 km/h
Hence, the answer is option (1).
$V_{A B}=\sqrt{V_A^2+V_B^2+2 V_A V_B \cos (180-\theta)}$
Example 2: Person A is moving along east and B is moving along north. The relative velocity of A concerning B is :$(\left.V_A=10 \mathrm{~m} / \mathrm{s}, V_B=10 \sqrt{3} \mathrm{~m} / \mathrm{s}\right)$
1) 20 m/s along north
2) 20 m/s along south
3) 20 m/s along 1200 with east
4) None of the above
Solution:
$\begin{aligned}
& \overrightarrow{V_A}=\text { Velocity of object } A \text {. } \\
& \overrightarrow{V_B}=\text { Velocity of object } B .
\end{aligned}$
$\text { The relative velocity of } \mathrm{B} \text { wrt to } \mathrm{A} \text { is } V_{BA}$
$\begin{aligned}
& \overrightarrow{V_{B / A}}=\overrightarrow{V_B} \cdot \overrightarrow{V_A}=10 \sqrt{3} \hat{j}-10 \hat{\imath} \\
& \left|\overrightarrow{V_{B / A}}\right|=\sqrt{100+300}=20 \mathrm{~m} / \mathrm{s} \\
& \tan \theta=\frac{V_B}{V_A}=\frac{10 \sqrt{3}}{10}=\sqrt{3} \\
& \text { So } \theta=60^{\circ} \text { from west } \\
& \text { i.e } \theta=120^{\circ} \text { from east }
\end{aligned}$
Hence, the answer is option (3).
Related Topics:
Example 3: Rain is falling vertically downward with a speed of 4 km/h. A girl moves on a straight road with a velocity of 3km/h. The apparent speed (in m/s) of rain with respect to the girl is:
1) 5
2) 4
3) 3
4) 7
Solution :
$
\overrightarrow{V_{R / G}}=\overrightarrow{V_R}-\overrightarrow{V_G}
$
$\mathrm{V}_{\mathrm{R}}=$ Velocity of rain wrt ground, $\mathrm{V}_{\mathrm{G}}=$ Velocity of girl wrt ground
$
\left|\overrightarrow{V_{R / G}}\right|=\sqrt{V_R^2+V_G^2}=\sqrt{3^2+4^2}=5 \mathrm{~km} / \mathrm{h}
$
Hence, the answer is option (1).
Example 4: A particle A is moving along north with a speed of 3 m/s and another particle B is moving with a velocity of 4 m/s at 60o with north, then the velocity of B as seen by A is
1) $5 \mathrm{~m} / \mathrm{s}$
2) $3.5 \mathrm{~m} / \mathrm{s}$
3) $\sqrt{13} \mathrm{~m} / \mathrm{s}$
4) $\sqrt{15} \mathrm{~m} / \mathrm{s}$
Solution:
The relative velocity of a body, A with respected body B when the two bodies moving at an angle $\theta$ is:
$\begin{aligned}
& V_{A B}=\sqrt{V_A^2+V_B^2+2 V_A V_B \cos (180-\theta)} \\
& =\sqrt{V_A^2+V_B^2-2 V_A V_B \cos (\theta)} \\
& \left|\vec{V}_{A B}\right|=\sqrt{V_A^2+V_B^2-2 V_A V_B \cdot \cos \theta} \\
& =\sqrt{3^2+4^2-2 \times 3 \times 4 \times \frac{1}{2}}=\sqrt{13} \mathrm{~m} / \mathrm{s} \\
&
\end{aligned}$
Hence, the answer is option (3).
Example 5: A particle A is moving along the x-axis and a particle B is moving along the y-axis. The speed of A is 6m/s and that of B is 8 m/s, then the velocity (in m/s) of A concerning B is:
1) 10
2) 12
3) 8
4) 14
Solution:
Relative Velocity of $\mathrm{A}$ with respect to $\mathrm{B}$ is
$
\begin{aligned}
& V_{A B}=\sqrt{V_A^2+V_B^2} \\
& V_{A B}=\sqrt{V_A^2+V_B^2}=\sqrt{8^2+6^2}=10 \mathrm{~m} / \mathrm{s}
\end{aligned}
$
Hence, the answer is option (1).
The length of the connecting rod is determined by the angular velocity of the crank, the radius of the crank, and the angular velocity of the crank.
Let us denote the motorcycle's velocity as VA and the car's velocity as VB.
VAB = VA – VB
We get VAB = 120 km/h – 90 km/h = 30 km/h by substituting the variables in the above equation.
As a result, the motorcycle's relative velocity to the car's passenger is 30 km/h.
The above statement is correct. Negative relative velocity is possible. It is possible for relative velocity to be negative because it is the difference between two velocities regardless of their magnitude.
The difference between velocity and relative velocity is that relative velocity is measured in relation to a reference point that is located at a different location. While absolute velocity is measured in a frame where an object is either at rest or moving with regard to the absolute frame, relative velocity is measured in a frame where an object is either at rest or moving with respect to the absolute frame.
The usage of relative velocity is necessary since it is needed to determine whether an object is at rest or moving.
It is the velocity of an object as observed from a particular reference frame that is also in motion. It is the difference between the velocities of two objects.
In riverboat problems, relative velocity helps determine the actual path and speed of the boat relative to the ground. If a boat is moving in a river with a current, the boat’s velocity relative to the ground is the vector sum of the boat’s velocity relative to the water and the river’s current velocity.
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