Hello, my dear students! Welcome to an exciting and super practical concept in Kinematics:
Relative Velocity in One Dimension. This topic is incredibly important, not just for your exams like JEE Mains and Advanced, but also for understanding how the world around you truly works. Have you ever wondered why a car moving next to you on a highway appears to be barely moving, even if both cars are zooming at 100 km/h? Or why it feels like an oncoming train rushes past you much faster than a train going in the same direction? The answer lies in
relative velocity!
Let's dive in and unlock this concept, starting from the very basics.
### The Foundation: What is Relative Velocity?
Imagine you're standing on a railway platform, watching a train go by. You'd say the train is moving at, say, 60 km/h. Now, imagine a person *inside* that train is walking towards the front of the train at 5 km/h. How fast is that person moving?
Well, it depends on who you ask!
* For you, standing on the platform, the person is moving at 60 km/h (speed of train) + 5 km/h (speed of person relative to train) = 65 km/h.
* For someone sitting on a seat *inside* the same train, that person is just walking at 5 km/h.
This simple example highlights a crucial point:
motion is relative. The velocity of an object depends on the
frame of reference from which it is observed.
Relative velocity is simply the velocity of an object as observed from another moving object (or frame of reference). It's all about how one object "sees" the motion of another.
### Understanding the Frame of Reference
Before we get into formulas, let's solidify the idea of a
frame of reference. Think of it as your observation point, a place from which you are measuring positions, distances, and velocities.
* When you say a car is moving at 60 km/h, you implicitly mean 60 km/h *with respect to the ground* (or the road, or the Earth). Your frame of reference is the ground, which we usually consider stationary.
* When the person inside the train says they are walking at 5 km/h, they mean *with respect to the train*. Their frame of reference is the train itself.
For our study of relative velocity, it's vital to always clearly define what we mean by "with respect to what".
### Building Intuition: A Simple Scenario
Let's consider two friends,
Car A and
Car B, driving on a straight highway. We'll use a positive sign for velocities to the right and a negative sign for velocities to the left.
Scenario |
Car A's Velocity (`v_A`) |
Car B's Velocity (`v_B`) |
How does A see B? (Velocity of B relative to A) |
How does B see A? (Velocity of A relative to B) |
|---|
Both moving right, A faster |
+100 km/h |
+80 km/h |
B moves left relative to A at 20 km/h |
A moves right relative to B at 20 km/h |
Both moving right, B faster |
+80 km/h |
+100 km/h |
B moves right relative to A at 20 km/h |
A moves left relative to B at 20 km/h |
Moving in opposite directions |
+80 km/h |
-100 km/h |
B moves left relative to A at 180 km/h |
A moves right relative to B at 180 km/h |
Both stationary |
0 km/h |
0 km/h |
B is stationary relative to A |
A is stationary relative to B |
Notice how in the first two scenarios, when they are moving in the *same* direction, the relative speed is the *difference* in their speeds. When they are moving in *opposite* directions, the relative speed is the *sum* of their speeds. This intuition will be key!
### Formalizing Relative Velocity in One Dimension
Let's denote the velocity of object A with respect to the ground (or a stationary observer) as
`v_A`, and the velocity of object B with respect to the ground as
`v_B`. Remember, in one dimension, these are essentially scalar values but carry a sign (+ or -) to indicate direction.
The velocity of object A with respect to object B, denoted as
`v_AB`, is given by:
`v_AB = v_A - v_B`
Similarly, the velocity of object B with respect to object A, denoted as
`v_BA`, is given by:
`v_BA = v_B - v_A`
From these definitions, you can clearly see that
`v_AB = -v_BA`. This makes perfect sense: if you see a friend walking forward at 5 km/h relative to you, then your friend sees you walking backward at 5 km/h relative to them!
#### Derivation (A quick look)
Imagine the positions of two objects A and B at any time `t` are `x_A(t)` and `x_B(t)` with respect to a common origin on the ground.
The position of A with respect to B, let's call it `x_AB(t)`, is given by:
`x_AB(t) = x_A(t) - x_B(t)`
Now, velocity is the rate of change of position with respect to time. So, if we differentiate this equation with respect to time:
`d(x_AB)/dt = d(x_A)/dt - d(x_B)/dt`
Which gives us:
`v_AB = v_A - v_B`
This derivation confirms our formula!
### Cases to Remember for 1D Relative Velocity
Let's re-examine our car scenarios with the formula:
1.
Objects Moving in the Same Direction (e.g., both right)
* Let `v_A = +100 km/h` and `v_B = +80 km/h`.
* Velocity of A relative to B: `v_AB = v_A - v_B = (+100) - (+80) = +20 km/h`. (B sees A moving ahead at 20 km/h)
* Velocity of B relative to A: `v_BA = v_B - v_A = (+80) - (+100) = -20 km/h`. (A sees B falling behind at 20 km/h)
Key takeaway: When objects move in the same direction, their relative speed is the absolute difference of their individual speeds.
2.
Objects Moving in Opposite Directions (e.g., A right, B left)
* Let `v_A = +80 km/h` and `v_B = -100 km/h` (negative because B is moving left).
* Velocity of A relative to B: `v_AB = v_A - v_B = (+80) - (-100) = +80 + 100 = +180 km/h`. (B sees A approaching/moving right at 180 km/h)
* Velocity of B relative to A: `v_BA = v_B - v_A = (-100) - (+80) = -100 - 80 = -180 km/h`. (A sees B approaching/moving left at 180 km/h)
Key takeaway: When objects move in opposite directions, their relative speed is the sum of their individual speeds.
### Important Notes for JEE & Competitive Exams
*
Always define your positive direction: This is crucial. Stick to a convention (e.g., right is positive, left is negative; up is positive, down is negative).
*
Specify the observer: Clearly identify who is observing whom. "Velocity of A with respect to B" is `v_A - v_B`, not `v_B - v_A`.
*
The 'ground' frame: Unless specified, `v_A` and `v_B` usually refer to velocities with respect to a stationary ground frame.
*
Relative Acceleration: Just like relative velocity, relative acceleration follows the same rule: `a_AB = a_A - a_B`. This becomes important in problems involving changing velocities.
*
Relative Displacement/Position: `x_AB = x_A - x_B` and `Ξx_AB = Ξx_A - Ξx_B`. This means the relative displacement is simply the difference in individual displacements.
### Practical Applications and Examples
Relative velocity simplifies many complex problems. For instance, if two trains are approaching each other, instead of calculating when they meet by considering both moving, you can fix one train and consider the other train approaching it with the *relative velocity*. This drastically simplifies the calculation to a simple `distance = relative speed Γ time` problem.
Let's work through a few examples to solidify your understanding.
Example 1: Cars on a Highway
Two cars, Car P and Car Q, are moving on a straight highway. Car P is moving at 70 km/h towards the East, and Car Q is moving at 50 km/h towards the East.
(a) What is the velocity of Car P with respect to Car Q?
(b) What is the velocity of Car Q with respect to Car P?
Solution:
Let's define East as the positive direction.
Velocity of Car P, `v_P = +70 km/h`
Velocity of Car Q, `v_Q = +50 km/h`
(a) Velocity of Car P with respect to Car Q (`v_PQ`):
`v_PQ = v_P - v_Q`
`v_PQ = (+70) - (+50) = +20 km/h`
This means Car Q observes Car P moving East (forward) at 20 km/h.
(b) Velocity of Car Q with respect to Car P (`v_QP`):
`v_QP = v_Q - v_P`
`v_QP = (+50) - (+70) = -20 km/h`
This means Car P observes Car Q moving West (backward) at 20 km/h. Car P sees Car Q falling behind.
Example 2: Meeting Trains
A train A is moving East at 90 km/h. Another train B is moving West at 72 km/h. They are initially 300 km apart.
(a) What is the velocity of train B with respect to train A?
(b) How much time will it take for them to meet?
Solution:
Let East be the positive direction.
Velocity of train A, `v_A = +90 km/h`
Velocity of train B, `v_B = -72 km/h` (since it's moving West)
(a) Velocity of train B with respect to train A (`v_BA`):
`v_BA = v_B - v_A`
`v_BA = (-72) - (+90) = -72 - 90 = -162 km/h`
This means train A observes train B approaching it from the West (moving in the negative direction) at a speed of 162 km/h. The relative speed of approach is 162 km/h.
(b) Time to meet:
The initial distance between them is `d = 300 km`.
The relative speed at which they are approaching each other is `|v_BA| = 162 km/h`.
Using the formula `time = distance / speed`:
`Time = d / |v_BA| = 300 km / 162 km/h`
`Time β 1.85 hours`
Example 3: Person on a Moving Walkway
A long moving walkway (like at an airport) moves at 3 m/s. A person walks on the walkway at a speed of 1 m/s relative to the walkway.
(a) What is the person's speed relative to the ground if they walk in the same direction as the walkway?
(b) What is the person's speed relative to the ground if they walk opposite to the direction of the walkway?
Solution:
Let the direction of the walkway be positive.
Velocity of walkway with respect to ground, `v_W = +3 m/s`
Velocity of person with respect to walkway, `v_PW = +1 m/s` (walking in same direction) or `-1 m/s` (walking opposite direction).
We need to find the velocity of the person with respect to the ground, `v_P`.
We know `v_PW = v_P - v_W`.
Rearranging, `v_P = v_PW + v_W`. This is a very common scenario - the absolute velocity is the sum of the velocity relative to the moving frame and the velocity of the moving frame itself.
(a) Person walks in the same direction as the walkway:
`v_PW = +1 m/s`
`v_P = (+1) + (+3) = +4 m/s`
The person's speed relative to the ground is 4 m/s in the direction of the walkway.
(b) Person walks opposite to the direction of the walkway:
`v_PW = -1 m/s`
`v_P = (-1) + (+3) = +2 m/s`
The person's speed relative to the ground is 2 m/s in the direction of the walkway (they are still moving forward, but slower). If `v_PW` was greater than `v_W`, they would move backward relative to the ground. For example, if they walked at 4 m/s opposite to the walkway, `v_P = (-4) + (+3) = -1 m/s` (moving backward at 1 m/s relative to ground).
### Conclusion for Fundamentals
You've now grasped the fundamental principles of relative velocity in one dimension! Remember, it all boils down to understanding:
1.
Frame of Reference: Who is observing?
2.
Vector Nature: Direction matters β use positive and negative signs consistently.
3.
The Formula: `v_AB = v_A - v_B` is your best friend.
This simple concept is a powerful tool for analyzing motion and will be extended to two and three dimensions, which you'll encounter soon. For JEE, problems often involve scenarios like these, sometimes combined with constant acceleration, so make sure your conceptual foundation here is rock solid!