Q.At a metro station, a girl walks up a stationary escalator in time t1. If she remains stationary on the escalator, then the escalator take her up in time t2. The time taken by her to walk up on the moving escalator will be
Imagine you're sitting in a train that's moving smoothly. The person sitting opposite you appears to be perfectly still — yet both of you are hurtling past trees and buildings outside at 80 km/h. Which is the "real" velocity? The answer is: there is no single real velocity. Velocity always depends on who is measuring it.
That's the core idea of relative velocity: the velocity of an object as seen from a particular frame of reference. Change the frame, and the measured velocity changes.
The Intuition: Walking on a Moving Train
Let's build this step by step.
Step 1 — You on a stationary train.
You walk forward at 3 km/h inside the aisle. A friend on the platform sees you moving at exactly 3 km/h. Simple.
Step 2 — The train moves at 80 km/h, you stand still inside.
Your friend on the platform sees you moving at 80 km/h (the train's speed). You see the platform rushing backward at 80 km/h.
Step 3 — You walk forward at 3 km/h while the train moves at 80 km/h.
Your friend on the platform sees you moving at 80+3=83 km/h.
But the person sitting next to you sees you moving at just 3 km/h.
Same you, same walking speed — two different observers, two different velocities. That's relative velocity in action.
Note
The "velocity" you feel is always relative to something. When you say "a car is moving at 60 km/h", you usually mean relative to the ground. But the ground itself is moving (Earth rotates, orbits the Sun, etc.). There is no absolute rest frame.
The Precise Definition
Relative velocity of object A with respect to object B is the velocity of A as measured by an observer who is at rest with respect to B.
Mathematically, if vA and vB are velocities of A and B measured in the same frame (say, the ground), then:
vAB=vA−vB
Where vAB means "velocity of A relative to B".
Read this carefully: you subtract the velocity of the reference object (B) from the velocity of the object you're tracking (A).
Why Subtraction? — The Logic
Think of the train example again. Let:
vyou = your velocity relative to ground = 83 km/h forward
vtrain = train's velocity relative to ground = 80 km/h forward
Your velocity relative to the train is:
vyou,train=vyou−vtrain=83−80=3 km/h forward
That matches: the person on the train sees you walking forward at 3 km/h.
Now what about the platform's velocity relative to you?
Platform is at rest relative to ground: vplatform=0
vplatform, you=0−83=−83 km/h
The negative sign means the platform appears to move backward relative to you — which is exactly what you see from the moving train.
Watch out
A common mistake: thinking relative velocity is just adding speeds. It's vector subtraction. If two objects move in opposite directions, you subtract a negative — which becomes addition. Always use the vector formula.
One-Dimensional Cases (The Simplest)
When motion is along a straight line, we can use signs (+ for one direction, − for the opposite).
Concept: Relative velocity – when the girl walks on the moving escalator, her effective speed is the sum of her walking speed and the escalator's speed.
Let the length of the escalator be L.
Step 1: The girl's walking speed (escalator stationary) is vg=t1L.
Step 2: The escalator's speed (girl stationary) is ve=t2L.
Step 3: When she walks up the moving escalator, both speeds add:
When the girl walks on the moving escalator, her speed and the escalator's speed add; since speed is distance over time, the combined rate is the sum of individual rates, giving time t1+t2t1t2.
The key insight is that speeds add when motions are in the same direction. When you walk on a moving walkway, you cover ground faster than either you or the walkway alone would manage. The natural language here is rates: if the girl climbs at a certain rate (escalator-lengths per unit time) and the escalator moves at its own rate, the combined rate is simply the sum.
Let the length of the escalator be L.
When the girl walks up the stationary escalator in time t1, her walking speed is
vgirl=t1L.
When she stands still and the escalator carries her up in time t2, the escalator's speed is
vesc=t2L.
Now consider what happens when both move together.
The effective speed is the sum of the two speeds.
The girl walks at vgirl relative to the escalator, and the escalator itself moves at vesc relative to the ground. Relative to the ground, her speed is
Concept: Combined-Rate Reasoning, Verified by Limiting Cases
Method: Rate-Addition by Analogy, Checked at the Extremes (a "two workers" style argument, sanity-checked rather than re-derived from scratch)
This treats the problem as a "combined rate" problem — the same structure as two people working together, or two pipes filling a tank — and, crucially, verifies the resulting formula by checking it against physically obvious extreme cases, rather than only deriving it once through algebra.
Steps
Express each rate as "escalator-lengths per unit time." If the escalator has length L: the girl's own walking rate (escalator off) is t11 (in units of L per unit time), and the escalator's own rate (girl standing still) is t21.
Combined rates add, exactly as with two workers or two taps filling the same tank together:
combined rate=t11+t21=t1t2t1+t2
Time is the reciprocal of the combined rate (to cover one full escalator length, L=1 in these units):
t=combined rate1=t1+t2t1t2
Sanity-check by taking t1→∞ (the girl walks so slowly it's as if she isn't walking at all): the formula should reduce to "just ride the escalator," i.e. t→t2.
Sanity-check by taking t2→∞ (the escalator is effectively stationary): the formula should reduce to "just walk," i.e. t→t1.
limt2→∞t1+t2t1t2=limt2→∞1+t1/t2t1=t1✓ …