Prerequisites
Before studying this topic, make sure you understand:
- Frame of Reference - reference frames concept
- Motion in a Plane - vector addition
What is Relative Velocity?
Relative velocity is the velocity of one object as observed from another moving object.
The Formula
The velocity of object A relative to object B:
$$\boxed{\vec{v}_{AB} = \vec{v}_A - \vec{v}_B}$$Similarly:
$$\vec{v}_{BA} = \vec{v}_B - \vec{v}_A = -\vec{v}_{AB}$$Important Properties
- $\vec{v}_{AB} + \vec{v}_{BA} = 0$
- $\vec{v}_{AB} = -\vec{v}_{BA}$ (equal magnitude, opposite direction)
- $\vec{v}_{AC} = \vec{v}_{AB} + \vec{v}_{BC}$ (chain rule)
Cases in 1D Motion
Same Direction
If A and B move in the same direction:
$$v_{AB} = v_A - v_B$$Example: Car A at 80 km/h, Car B at 60 km/h (same direction)
- A relative to B: 80 - 60 = 20 km/h (A appears to move forward)
- B relative to A: 60 - 80 = -20 km/h (B appears to move backward)
Opposite Directions
If A and B move in opposite directions:
$$|v_{AB}| = v_A + v_B$$Example: Two trains approaching each other at 60 km/h each
- Relative speed = 60 + 60 = 120 km/h
- Same direction: Subtract speeds
- Opposite directions: Add speeds
Cases in 2D Motion
For 2D motion, use vector subtraction:
$$\vec{v}_{AB} = \vec{v}_A - \vec{v}_B$$Magnitude: $|\vec{v}_{AB}| = \sqrt{v_A^2 + v_B^2 - 2v_Av_B\cos\theta}$
where $\theta$ is the angle between $\vec{v}_A$ and $\vec{v}_B$.
Special cases:
- $\theta = 0°$ (same direction): $|v_{AB}| = |v_A - v_B|$
- $\theta = 180°$ (opposite): $|v_{AB}| = v_A + v_B$
- $\theta = 90°$ (perpendicular): $|v_{AB}| = \sqrt{v_A^2 + v_B^2}$
Interactive Demo: Visualize Vector Addition
See how relative velocity is calculated using vector subtraction.
Application 1: Rain and Man Problem
Problem Setup
A man walks with velocity $\vec{v}_m$ while rain falls with velocity $\vec{v}_r$. What angle does the rain appear to fall?
Solution Approach
Velocity of rain relative to man:
$$\vec{v}_{rm} = \vec{v}_r - \vec{v}_m$$The rain appears to come from the direction of $\vec{v}_{rm}$.
Common Scenarios
Case 1: Rain falling vertically, man walking horizontally
If rain falls at speed $v_r$ (vertical) and man walks at $v_m$ (horizontal):
$$|\vec{v}_{rm}| = \sqrt{v_r^2 + v_m^2}$$Angle with vertical: $\tan\alpha = \frac{v_m}{v_r}$
To stay dry: The man should hold his umbrella at angle $\alpha$ from vertical, tilted forward.
Case 2: At what speed should man walk so rain appears vertical?
Man should walk with velocity equal to the horizontal component of rain velocity.
Application 2: River Crossing
A boat crosses a river of width $d$ with current velocity $\vec{v}_r$.
Problem Types
Type 1: Shortest Time
Point boat directly across (perpendicular to bank).
- Time: $t = \frac{d}{v_b}$
- Drift: $x = v_r \times t = \frac{v_r \cdot d}{v_b}$
Type 2: Shortest Path (No Drift)
Point boat upstream at angle $\theta$ such that:
$$v_b\sin\theta = v_r$$ $$\sin\theta = \frac{v_r}{v_b}$$This requires $v_b > v_r$ (boat faster than current).
- Resultant velocity: $v_{res} = \sqrt{v_b^2 - v_r^2}$
- Time: $t = \frac{d}{\sqrt{v_b^2 - v_r^2}}$
Summary Table
| Objective | Boat Direction | Time | Drift |
|---|---|---|---|
| Shortest time | Perpendicular | $\frac{d}{v_b}$ | $\frac{v_r d}{v_b}$ |
| Shortest path | Upstream at $\sin^{-1}(\frac{v_r}{v_b})$ | $\frac{d}{\sqrt{v_b^2 - v_r^2}}$ | 0 |
Application 3: Aircraft in Wind
For an aircraft with airspeed $\vec{v}_a$ flying in wind $\vec{v}_w$:
Ground velocity: $\vec{v}_g = \vec{v}_a + \vec{v}_w$
To reach destination directly
The pilot must head at an angle such that the resultant velocity points toward the destination.
Practice Problems
Two cars A and B move with velocities 20 m/s east and 15 m/s north respectively. Find velocity of A relative to B.
Solution: $\vec{v}_A = 20\hat{i}$ m/s, $\vec{v}_B = 15\hat{j}$ m/s
$\vec{v}_{AB} = \vec{v}_A - \vec{v}_B = 20\hat{i} - 15\hat{j}$ m/s
$|\vec{v}_{AB}| = \sqrt{20^2 + 15^2} = \sqrt{625} = $ 25 m/s
Direction: $\tan\theta = \frac{15}{20} = 0.75$, $\theta = 36.87°$ south of east
Rain falls vertically at 10 m/s. A man walks at 6 m/s. At what angle should he hold his umbrella?
Solution: $\tan\alpha = \frac{v_m}{v_r} = \frac{6}{10} = 0.6$
$\alpha = \tan^{-1}(0.6) ≈ $ 31° from vertical (tilted forward)
A river is 400 m wide with current 3 m/s. A boat has speed 5 m/s in still water. Find: (a) Time for shortest path (b) Time for shortest time
Solution: (a) $v_{res} = \sqrt{5^2 - 3^2} = 4$ m/s $t = \frac{400}{4} = $ 100 s
(b) $t = \frac{400}{5} = $ 80 s (with drift = $\frac{3 \times 400}{5} = 240$ m)