Mechanics

Forces & Newton's Laws

Year 12 · Year 13

  • Calculate the resultant force acting on an object and determine its effect on motion.
  • Apply Newton's Second Law (F=ma) to solve problems involving constant acceleration in one or two dimensions.
  • Analyse and solve problems involving connected particles, such as those linked by strings or in contact.
  • Model and solve problems involving friction on both horizontal and inclined planes.

Key concepts

Resultant Force

The single force that has the same effect as all the individual forces acting on an object. It is the vector sum of all forces. If the resultant force is zero, the object is in equilibrium (at rest or moving with constant velocity).

Newton's First Law of Motion

An object remains at rest or continues to move with constant velocity unless acted upon by a resultant external force. This is also known as the law of inertia.

Newton's Second Law of Motion

The resultant force acting on an object is directly proportional to its mass and its acceleration, and acts in the same direction as the acceleration.

F = ma
Newton's Third Law of Motion

For every action, there is an equal and opposite reaction. When object A exerts a force on object B, object B simultaneously exerts an equal and opposite force on object A. These forces act on different objects.

Weight (W)

The force of gravity acting on an object. It always acts vertically downwards towards the centre of the Earth.

W = mg
Normal Reaction (R)

The force exerted by a surface on an object in contact with it, acting perpendicularly away from the surface. It prevents the object from passing through the surface.

Tension (T)

The force transmitted through a string, rope, cable, or similar one-dimensional continuous object when pulled tight by forces acting from opposite ends. It acts along the string, away from the object.

Friction (F_f)

A force that opposes the relative motion or tendency of motion between two surfaces in contact. It acts parallel to the surfaces. For limiting friction (when an object is on the point of moving or is moving), F_f = μR.

F_f ≤ μR
Coefficient of Friction (μ)

A dimensionless scalar quantity that describes the ratio of the force of friction between two bodies and the force pressing them together. It depends on the nature of the surfaces in contact.

μ = F_f / R
Connected Particles

A system of two or more objects that are linked together, often by a string or in direct contact. They typically share the same acceleration (if moving together) or have related accelerations. Forces like tension or contact forces act between them.

Inclined Planes

A flat surface tilted at an angle to the horizontal. When an object is on an inclined plane, its weight needs to be resolved into components parallel and perpendicular to the plane to apply Newton's laws effectively.

Key facts to remember

  • 1Newton's First Law: An object remains in its state of motion unless a resultant force acts on it.
  • 2Newton's Second Law: F = ma, where F is the resultant force, m is mass, and a is acceleration. This is a vector equation.
  • 3Newton's Third Law: For every action, there is an equal and opposite reaction.
  • 4Weight (W) = mg, where g is the acceleration due to gravity (approximately 9.8 m/s²).
  • 5Friction (F_f) opposes motion or the tendency of motion and its maximum value is F_f = μR, where μ is the coefficient of friction and R is the normal reaction.
  • 6When resolving forces on an inclined plane, resolve weight into components parallel (mg sinθ) and perpendicular (mg cosθ) to the plane.
  • 7For connected particles, apply F=ma to each particle separately, remembering that tension in a light inextensible string is uniform and acceleration is shared.
  • 8Always draw a clear force diagram and choose a consistent positive direction for each object.

Worked examples

Example 1

A particle of mass 5 kg is acted upon by two forces, F₁ = (3i + 7j) N and F₂ = (2i - 3j) N. Find the acceleration of the particle.

IFind the resultant force R = F₁ + F₂.
IIR = (3i + 7j) + (2i - 3j)
IIIR = (3+2)i + (7-3)j
IVR = (5i + 4j) N
VApply Newton's Second Law, F = ma.
VI(5i + 4j) = 5a
VIISolve for acceleration a.
VIIIa = (5i + 4j) / 5
9a = (1i + 0.8j) m/s²

Answer

The acceleration of the particle is (i + 0.8j) m/s².

Forces and acceleration are vector quantities.

Example 2

A particle P of mass 3 kg and a particle Q of mass 2 kg are connected by a light inextensible string. The string passes over a smooth fixed pulley. The system is released from rest. Find the acceleration of the particles and the tension in the string.

IDraw a clear diagram showing the forces acting on each particle.
IIFor P (3 kg): Weight (3g N) downwards, Tension (T N) upwards.
IIIFor Q (2 kg): Weight (2g N) downwards, Tension (T N) upwards.
IVChoose a positive direction for acceleration. Let's assume P moves downwards and Q moves upwards.
VApply Newton's Second Law (F=ma) to particle P:
VIForces acting on P: 3g (downwards), T (upwards).
VIIEquation for P: 3g - T = 3a (Equation 1)
VIIIApply Newton's Second Law (F=ma) to particle Q:
9Forces acting on Q: T (upwards), 2g (downwards).
10Equation for Q: T - 2g = 2a (Equation 2)
11Solve the simultaneous equations for a and T.
12Add (1) and (2):
13(3g - T) + (T - 2g) = 3a + 2a
14g = 5a
15a = g/5
16Using g = 9.8 m/s²: a = 9.8 / 5 = 1.96 m/s²
17Substitute 'a' back into Equation 2 to find T:
18T - 2g = 2(g/5)
19T = 2g + 2g/5
20T = 10g/5 + 2g/5
21T = 12g/5
22T = 12(9.8)/5 = 23.52 N

Answer

The acceleration of the particles is 1.96 m/s² and the tension in the string is 23.5 N (3 s.f.).

"Light inextensible string" means tension is uniform throughout and particles have the same magnitude of acceleration. "Smooth pulley" means no friction at the pulley.

Example 3

A block of mass 4 kg rests on a rough plane inclined at an angle of 30° to the horizontal. The coefficient of friction between the block and the plane is 0.2. A force P N acts on the block, parallel to the plane and directed up the plane. Find the minimum value of P required to prevent the block from sliding down the plane.

IDraw a diagram showing all forces acting on the block.
IIWeight (4g N) vertically downwards.
IIINormal Reaction (R N) perpendicular to the plane, upwards.
IVForce P (P N) parallel to the plane, upwards.
VFriction (F_f N) parallel to the plane, upwards (as the block is on the point of sliding *down*, friction opposes this motion by acting *up* the plane).
VIResolve the weight into components parallel and perpendicular to the plane.
VIIComponent perpendicular to plane: 4g cos 30°
VIIIComponent parallel to plane: 4g sin 30° (acting down the plane)
9Apply Newton's Second Law (F=ma) perpendicular to the plane. Since there is no acceleration perpendicular to the plane, the forces are in equilibrium.
10R - 4g cos 30° = 0
11R = 4g cos 30°
12R = 4(9.8) * (√3 / 2) = 19.6√3 N ≈ 33.948 N
13Determine the maximum static friction (limiting friction) when the block is on the point of sliding.
14F_f = μR = 0.2 * (19.6√3) = 3.92√3 N ≈ 6.790 N
15Apply Newton's Second Law (F=ma) parallel to the plane. For the minimum P to prevent sliding down, the block is in limiting equilibrium, so acceleration is 0. Forces acting up the plane balance forces acting down the plane.
16Forces up the plane: P + F_f
17Forces down the plane: 4g sin 30°
18P + F_f = 4g sin 30°
19P + 3.92√3 = 4(9.8) * (1/2)
20P + 3.92√3 = 19.6
21P = 19.6 - 3.92√3
22P ≈ 19.6 - 6.790 = 12.81 N

Answer

The minimum value of P required is 12.8 N (3 s.f.).

Always consider the direction of impending motion to determine the direction of friction.

Common mistakes

  • Confusing mass (scalar, in kg) with weight (vector force, in N).
  • Incorrectly resolving forces, especially the weight component on an inclined plane (e.g., using sinθ for the perpendicular component).
  • Forgetting to include the normal reaction force or friction force when appropriate.
  • Making sign errors when setting up F=ma equations, particularly when forces act in opposite directions.
  • Assuming tension in a string is always equal to the weight of a hanging mass in a pulley system when the system is accelerating.

Exam tips

  • Always start by drawing a clear, labelled diagram showing all forces acting on each object in the system.
  • Choose a consistent positive direction for acceleration and forces for each object, especially in connected particle problems.
  • When dealing with inclined planes, resolve forces parallel and perpendicular to the plane.
  • Clearly state any assumptions made (e.g., "light inextensible string", "smooth pulley", "particle").
  • Use g = 9.8 m/s² unless specified otherwise, and give answers to an appropriate number of significant figures (usually 3 s.f.).

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