Pulley in Physics (original) (raw)

Last Updated : 17 Feb, 2026

A pulley is a simple machine that is made up of a wheel and a rope or cable that helps us to lift heavy objects more easily. The wheel rotates freely around the axle, and it is generally made up of wood, metal, or even plastic for lifting lighter loads.

pulley_5

The main function of a pulley is to change the direction of force. Instead of lifting a heavy object directly upward, you can pull the rope downward to raise the load. This makes lifting easier and convenient; that's why pulleys are used in wells, cranes, elevators, and flagpoles.

**Mechanical Advantage:

Mechanical advantage tells us how much easier a pulley makes in lifting a load. It is the ratio of the weight being lifted (load) to the force you apply (effort).
M = \frac{W}{F}

In other words, we can say it tells us how many times the pulley reduces our effort. The greater the mechanical advantage, the less force you need to lift the same weight.

Types of Pulley

types_of_pulleys

1. Fixed Pulley

2. Movable Pulley

3. Compound Pulley

4. Block and Tackle

**Effect of Number of Pulleys on Mechanical Advantage

pulley_2

To lift a 1 kg weight in this rope pulley setup, we have to apply a force equal to the weight itself: F=W

The rope tension is the same as the applied force, so there’s no reduction in effort.

So, the mechanical advantage is 1. To lift the weight by 1 ft, you pull 1 ft of rope.

pulley_3

To lift a 1 kg weight using a simple two-pulley system, the rope tension equals the force you apply (F). But the weight is supported by two segments of the rope, so: 2T=W

This means you only need to apply half the force: F = \frac{W}{2}

So the mechanical advantage is 2. To lift the weight 1 ft, you must pull 2 ft of rope.

**More Pulley arrangements

pulley

String Constraint Method

In pulley problems, the total length of the string attached to the pulley remains constant (if the string is ideal and inextensible). This condition gives us a mathematical relation between the displacement, velocity, and acceleration of different blocks attached to the system.

Since string length remains constant: L = x_1 + x_2 + \text{constant}

Differentiating: v_1 + v_2 = 0

Again differentiating: a_1 + a_2 = 0

For movable pulley: a_{block} = 2a_{pulley}

Ideal Pulley vs Real Pulley

a. Ideal Pulley System

In this case:

b. Real (Massive) Pulley

If the pulley has mass M and radius R, then tensions on two sides are not equal.

We must apply rotational dynamics.

\tau = I\alpha

(T_1 - T_2)R = I\alpha

Since the string does not slip: a = \alpha R

For a solid disc pulley: I = \frac{1}{2}MR^2

Therefore,

(T_1 - T_2)R = \frac{1}{2}MR^2 \cdot \frac{a}{R}

T_1 - T_2 = \frac{1}{2}Ma

Solved Questions

**Question 1:- Find the Tension (T) in the string and also the acceleration of the block.

ques_1

**Solution 1:

sol_1

m1 > m2

now for mass m1,

m1 g – T = m1a .........(i)

for mass m2

T – m2 g = m2 a .........(ii)

Adding (i) and (ii), we get

\mathbf{a}=\frac{(m_{1}-m_{2})}{(m_{1}+m_{2})}g

\mathbf{T}=\frac{2m_{1}m_{2}}{(m_{1}+m_{2})}g

**Question 2:- Find the Tension (T) in the string and also the acceleration of the block.

ques_2

**Solution 2:

sol_2

(m1 > m2)

m1g – T1 = m1a .........(i)

T2 – m2g = m2a .........(ii)

T1 – T2 = Ma .........(iii)

by (i), (ii) and (iii)

a=\frac{(m_{1}-m_{2})}{(m_{1}+m_{2}+M)}g

**Question 3:- Find the Tension (T) in the string and also the acceleration of the block.

ques_3

**Solution 3:

sol_3

For mass m1 : m1g – T = m1 a

For mass m2 : T – m2g sinθ = m2 a

\mathbf{a}=\frac{(m_{1}-m_{2}\sin \theta )}{(m_{1}+m_{2})}\mathbf{g}

\mathbf{T}=\frac{m_{1}m_{2}(1+\sin \theta )}{(m_{1}+m_{2})}\mathbf{g}

Unsolved Questions

**Question 1:- In the figure given below, with what acceleration will the block of mass m move? (Pulley and strings are massless and frictionless)

unsolved_1

**Question 2:- In the arrangement as shown, tension T 2 is (g = 10m/s 2 ).

unsolved_2