Atwood Machine Calculator

Find acceleration and rope tension for two masses connected over an ideal pulley

Parameters

kgⓘ
kgⓘ
kgⓘ
Set 0 for ideal pulley (ignored in calculation)
Show Trail

Controls

xⓘ

Calculated Values

Acceleration:
2.45;m/s22.45;m/s²
Tension:
36.79;N36.79;N
Net Force on System:
19.62;N19.62;N
Mass Difference:
2.00;kg(+→m1descends)2.00;kg (+ → m₁ descends)

Examples

5 kg and 3 kg

Standard Atwood machine.

  • Acceleration: 2.452.45
  • Tension: 29.4329.43

Visualization

The Atwood Machine

An Atwood machine has two masses connected by a string over a pulley. Ideal assumptions: massless string, frictionless pulley, no air drag.

Both masses share the same magnitude of acceleration a (string inextensible). Heavier mass accelerates downward if m₁ > m₂.

From Newton’s second law on each mass and eliminating tension: a = g(m₁ − m₂)/(m₁ + m₂). Equal masses → a = 0 (equilibrium).

String tension T = 2m₁m₂g/(m₁ + m₂). T is always between m₂g and m₁g when m₁ > m₂ and the system accelerates.

Real pulleys have rotational inertia and friction; this calculator uses the ideal model (pulley mass input is for reference only).

Key Concepts

  • a = g(m₁ − m₂)/(m₁ + m₂) — acceleration
  • T = 2m₁m₂g/(m₁ + m₂) — string tension
  • Same |a| for both masses
  • Equal masses: static equilibrium
  • Heavier mass descends (standard setup)
  • Ideal pulley: same T on both sides

Real-World Applications

  • Introductory lab measurement of g
  • Teaching Newton’s second law
  • Elevator counterweight analogy
  • Dynamics of connected bodies
  • JEE/NEET pulley systems (basic case)

Explore Further

More mechanics tools

Physics Equations

Acceleration:
a=gm1−m2m1+m2a = g\frac{m_1 - m_2}{m_1 + m_2}
Tension:
T=2m1m2gm1+m2T = \frac{2m_1 m_2 g}{m_1 + m_2}

Step-by-Step Solution

See how the main results are calculated.

1

Draw Free-Body Diagrams

For each mass: weight mg down, tension T up. Heavier mass accelerates down.

Equation:

m1g−T=m1a,T−m2g=m2am_1 g - T = m_1 a, \quad T - m_2 g = m_2 a

Calculation:

m1=5 kg,m2=3 kgm_1 = 5 \text{ kg}, \quad m_2 = 3 \text{ kg}

Result:

Two equations, two unknowns (T and a)

Explanation:

Assume m₁ > m₂ so m₁ descends. String is inextensible → |a₁| = |a₂| = a. Ideal pulley → same tension on both sides.

2

Solve for Acceleration

Add the two equations to eliminate T:

Equation:

a=gm1−m2m1+m2a = g\frac{m_1 - m_2}{m_1 + m_2}

Calculation:

a=9.81×5−35+3a = 9.81 \times \frac{5 - 3}{5 + 3}
a=2.45 m/s2a = 2.45 \text{ m/s}^2

Result:

a=2.45 m/s2a = 2.45 \text{ m/s}^2

Explanation:

Net driving force on the system = |m₁ − m₂|g = 19.62 N. Total inertia = m₁ + m₂.

3

Calculate String Tension

Substitute a into either force equation:

Equation:

T=2m1m2gm1+m2T = \frac{2m_1 m_2 g}{m_1 + m_2}

Calculation:

T=2(5)(3)(9.81)5+3=36.79 NT = \frac{2(5)(3)(9.81)}{5 + 3} = 36.79 \text{ N}

Result:

T=36.79 NT = 36.79 \text{ N}

Explanation:

T is between m₂g = 29.43 N and m₁g = 49.05 N. Equal masses → a = 0, T = mg.

Frequently Asked Questions (FAQ)

What if masses are equal?

Acceleration is zero and tension T = mg for either mass—the system is in equilibrium.

Is tension equal on both sides?

Yes for an ideal massless pulley and massless string.

Why is a smaller than g?

The net driving force is (m₁ − m₂)g but total inertia is (m₁ + m₂), so a < g.

Can the lighter mass accelerate upward?

Yes—if it is on the side that rises when the heavier mass descends.

Practice MCQs

  1. Heavier mass is 5 kg, lighter 3 kg. Heavier mass:
  2. Equal masses give acceleration:
  3. Tension in accelerating Atwood machine is: