Newton's Laws of Motion

Newton's three laws at A-Level depth; connected bodies; pulleys and inclined planes

# Newton's Laws of Motion — A-Level Physics

Newton's Laws are the foundation of classical mechanics. At A-Level, you need to apply these laws quantitatively to solve problems involving connected bodies, pulleys, inclined planes, and multi-force systems.


1. Newton's First Law

An object remains at rest or moves with constant velocity unless acted upon by a resultant force.

At A-Level depth:

  • Defines inertial reference frames — frames where the law holds
  • An object in equilibrium (F=0\sum \vec{F} = 0) has zero acceleration
  • Constant velocity includes both constant speed AND constant direction

2. Newton's Second Law

Fnet=ma\boxed{\vec{F}_{\text{net}} = m\vec{a}}

More generally (momentum form): F=dpdt=d(mv)dt\vec{F} = \frac{d\vec{p}}{dt} = \frac{d(m\vec{v})}{dt}

For constant mass: F=maF = ma

Vector equation: Apply separately in each direction.


3. Newton's Third Law

When object A exerts a force on object B, object B exerts an equal and opposite force on object A.

The two forces:

  • Are equal in magnitude
  • Opposite in direction
  • Act on different objects
  • Are the same type of force

4. Connected Bodies and Pulleys

Atwood Machine (Two Masses on a Pulley)

Masses m1m_1 (heavier) and m2m_2 connected by a light, inextensible string over a frictionless, massless pulley.

For m1m_1 (going down): m_1 g - T = m_1 a \tag{1}

For m2m_2 (going up): T - m_2 g = m_2 a \tag{2}

Add equations (1) and (2): m1gm2g=(m1+m2)am_1 g - m_2 g = (m_1 + m_2)a a=(m1m2)gm1+m2\boxed{a = \frac{(m_1 - m_2)g}{m_1 + m_2}}

T=2m1m2gm1+m2\boxed{T = \frac{2m_1 m_2 g}{m_1 + m_2}}

Body on a Table Connected to Hanging Mass

Mass m1m_1 on a frictionless table, connected by a string over the edge to hanging mass m2m_2.

For m1m_1 (horizontal): T=m1aT = m_1 a

For m2m_2 (vertical): m2gT=m2am_2 g - T = m_2 a

Adding: m2g=(m1+m2)am_2 g = (m_1 + m_2)a a=m2gm1+m2a = \frac{m_2 g}{m_1 + m_2}


5. Inclined Planes

For a mass mm on a slope at angle θ\theta:

Resolve weight along and perpendicular to the slope:

  • Along slope (down): mgsinθmg\sin\theta
  • Perpendicular to slope: mgcosθmg\cos\theta

Normal reaction: N=mgcosθN = mg\cos\theta

Without friction: ma=mgsinθma = mg\sin\thetaa=gsinθa = g\sin\theta

With friction (μ\mu): ma=mgsinθμmgcosθma = mg\sin\theta - \mu mg\cos\theta a=g(sinθμcosθ)a = g(\sin\theta - \mu\cos\theta)

The object accelerates down if tanθ>μ\tan\theta > \mu.


Worked Example: Atwood Machine

Problem

Masses of 5 kg and 3 kg are connected over a pulley. Find the acceleration and tension.

a=(53)×9.815+3=19.628=2.45 m/s2a = \frac{(5-3) \times 9.81}{5+3} = \frac{19.62}{8} = 2.45 \text{ m/s}^2

T=2×5×3×9.818=294.38=36.8 NT = \frac{2 \times 5 \times 3 \times 9.81}{8} = \frac{294.3}{8} = 36.8 \text{ N}

Solution

Worked Example: Inclined Plane with Friction

Problem

A 10 kg block is on a 30° slope with μ=0.2\mu = 0.2. Find the acceleration.

a=g(sin30°0.2cos30°)=9.81(0.50.2×0.866)=9.81(0.50.173)=9.81×0.327=3.21 m/s2a = g(\sin30° - 0.2\cos30°) = 9.81(0.5 - 0.2 \times 0.866) = 9.81(0.5 - 0.173) = 9.81 \times 0.327 = 3.21 \text{ m/s}^2

Solution

Worked Example: Two Bodies Connected

Problem

A 4 kg block on a frictionless table is connected to a 2 kg hanging mass. Find the acceleration and tension.

a=m2gm1+m2=2×9.814+2=3.27 m/s2a = \frac{m_2 g}{m_1 + m_2} = \frac{2 \times 9.81}{4 + 2} = 3.27 \text{ m/s}^2 T=m1a=4×3.27=13.1 NT = m_1 a = 4 \times 3.27 = 13.1 \text{ N}

Solution

Worked Example: Lift Problem

Problem

A 70 kg person stands on scales in a lift accelerating upwards at 2 m/s². What do the scales read?

The scales read the normal force NN: Nmg=maN - mg = ma N=m(g+a)=70(9.81+2)=70×11.81=826.7 NN = m(g + a) = 70(9.81 + 2) = 70 \times 11.81 = 826.7 \text{ N}

Apparent weight = 826.7 N (more than the actual weight of 686.7 N).


Solution

7. Practice Questions

    1. A 12 kg block is pulled along a rough horizontal surface by a 50 N force at 20° above the horizontal. The coefficient of friction is 0.3. Calculate the acceleration. (5 marks)
    1. Masses of 8 kg and 5 kg hang on opposite sides of a frictionless pulley. Calculate (a) the acceleration, (b) the tension. (4 marks)
    1. A 15 kg block on a 40° incline is connected by a string over a pulley to a 10 kg hanging mass. The surface is frictionless. Find the acceleration and determine which way the system moves. (5 marks)

    Answers

    1. Horizontal: 50cos20°μN=12a50\cos20° - \mu N = 12a. Vertical: N+50sin20°=12gN + 50\sin20° = 12gN=117.7217.10=100.62N = 117.72 - 17.10 = 100.62 N. 47.00.3(100.62)=12a47.0 - 0.3(100.62) = 12a47.030.2=12a47.0 - 30.2 = 12aa=1.40a = 1.40 m/s².
    1. (a) a=(85)(9.81)/(8+5)=29.43/13=2.26a = (8-5)(9.81)/(8+5) = 29.43/13 = 2.26 m/s². (b) T=2(8)(5)(9.81)/13=60.4T = 2(8)(5)(9.81)/13 = 60.4 N.

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Summary

  • N1: No resultant force → no acceleration
  • N2: F=maF = ma (apply in each direction independently)
  • N3: Equal and opposite forces on different objects
  • Connected bodies: Write F=maF = ma for each body; tension is internal force
  • Pulleys: a=(m1m2)g/(m1+m2)a = (m_1-m_2)g/(m_1+m_2)
  • Inclined planes: Resolve weight parallel and perpendicular to slope

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