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Mechanics: Dynamics and Kinematics

Year 1 / ASYear 2 / A-Level AQA, Edexcel, OCR, WJEC/Eduqas, CCEA

SUVAT equations, calculus kinematics, Newton's laws, connected particles, friction, inclined planes and projectiles - A-Level Maths mechanics (Edexcel 9MA0 Topics 17-18, AQA 7357 P-R) revised with worked examples and mark-scheme logic.

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🎯 Learning Objectives

📋 Key Definitions and Core Concepts

Kinematics: The study of motion without reference to forces: displacement, velocity, acceleration and time.
Dynamics: The study of motion with the forces causing it: Newton's laws, friction and connected systems.
Displacement: Position measured from a fixed origin in a stated positive direction; it can be negative, unlike distance travelled.
SUVAT equations: The five constant-acceleration formulae (v = u + at, s = ut + 1/2 at^2, s = 1/2 (u + v)t, v^2 = u^2 + 2as, s = vt - 1/2 at^2); valid only when acceleration is constant.
Newton's second law: The resultant force on a body equals its mass times its acceleration: F = ma, with F in newtons, m in kg, a in m/s^2.
Newton's third law: Forces between two interacting bodies are equal in magnitude, opposite in direction and of the same type - the basis of tension in connected particles.
Friction: A force opposing relative motion, of magnitude at most F = mu R, where mu is the coefficient of friction and R the normal reaction.
Coefficient of friction: The constant mu, with 0 <= mu; larger mu means rougher surfaces; friction takes any value up to mu R and reaches the maximum only in limiting equilibrium.
Projectile: A body moving under gravity alone: horizontal velocity constant (u cos(theta)), vertical acceleration -g, and the two motions treated independently.
Modelling assumptions: The idealisations stated in a question: light (massless) strings, inextensible, smooth (frictionless) pulleys, a particle (no size), no air resistance.

📌 Key Points

SUVAT (constant acceleration only): v = u + at, s = ut + 1/2 at^2, s = 1/2 (u + v)t, v^2 = u^2 + 2as, s = vt - 1/2 at^2 - pick the equation missing the quantity you do not need.
Calculus kinematics: v = ds/dt, a = dv/dt; backwards: s = integral of v dt, v = integral of a dt, with initial conditions fixing constants. Distance = integral of |v| dt.
Newton's second law: resultant force F = ma; weight = mg; resolve perpendicular and parallel to slopes (R = mg cos(theta), weight component mg sin(theta)).
Friction: at most F = mu R, opposing motion; reaches the maximum in limiting equilibrium. Connected particles: F = ma for each mass, solve simultaneously.
Projectiles: horizontal velocity u cos(theta) constant; vertical u sin(theta) with acceleration -g; at maximum height vertical velocity is 0.

Constant acceleration: the SUVAT equations

When acceleration is constant, five formulae connect the five quantities s (displacement), u (initial velocity), v (final velocity), a (acceleration) and t (time) (Edexcel 9MA0 Topic 17; AQA 7357 Q1-Q2; OCR A H640 22.01; WJEC/Eduqas and CCEA applied papers): v = u + at, s = ut + 1/2 at^2, s = 1/2 (u + v)t, v^2 = u^2 + 2as and s = vt - 1/2 at^2. Each formula misses one quantity, so the selection routine is: list what you know, list what you want, and use the equation that avoids the quantity you do not have. They are valid only for constant acceleration - a question switching to variable acceleration needs calculus, and using SUVAT there is a method error.

Two discipline points: choose a positive direction and stick to it (deceleration is a negative acceleration once a direction is fixed), and convert units before substituting (km/h to m/s by dividing by 3.6). Velocity-time graphs support the work: the gradient is the acceleration and the area under the graph is the displacement - useful checks and a source of graph questions.

Worked example: braking with SUVAT

A car travelling at 25 m/s brakes uniformly and comes to rest in 50 m. Find the deceleration and the braking time.

Line 1: u = 25, v = 0, s = 50, a unknown, t unknown. v^2 = u^2 + 2as avoids t (M1: correct selection).

Line 2: 0 = 25^2 + 2a(50) = 625 + 100a, so a = -6.25 m/s^2 (A1: deceleration 6.25 m/s^2).

Line 3: v = u + at: 0 = 25 - 6.25t, so t = 4 s (A1).

Note the sign: the acceleration is negative because it opposes the motion - an answer of 6.25 m/s^2 without the direction comment can lose the interpretation mark when the question asks for deceleration explicitly.

Variable acceleration: calculus kinematics

When acceleration is not constant, calculus takes over (Edexcel 9MA0 Topic 17; AQA 7357 Q3; OCR A H640 22.01): v = ds/dt and a = dv/dt differentiate downwards, while s = integral of v dt and v = integral of a dt integrate upwards, with initial conditions fixing the constants of integration. The chain r(t) -> v(t) -> a(t) runs downhill by differentiation and uphill by integration - know which direction the question demands.

The subtlety exam questions love: displacement versus distance. Displacement is the integral of v dt; distance is the integral of |v| dt - when the particle changes direction (v = 0), you must split the integral at the turning points and add the absolute values. Find where v = 0 first in any distance question.

Worked example: displacement versus distance

A particle moves with velocity v(t) = 3t^2 - 12t + 9 m/s. Find its displacement and the distance travelled from t = 0 to t = 3.

Line 1: s(t) = t^3 - 6t^2 + 9t (integral of v, s(0) = 0) (M1 A1).

Line 2: Displacement = s(3) - s(0) = 27 - 54 + 27 = 0 m (A1).

Line 3: v(t) = 3(t - 1)(t - 3), so v = 0 at t = 1 and t = 3 - the particle changes direction (M1: direction changes found).

Line 4: s(1) = 1 - 6 + 9 = 4. Distance = |s(1) - s(0)| + |s(3) - s(1)| = 4 + 4 = 8 m (A1: split at turning points).

Displacement zero with distance 8 m is the classic contrast: the particle returns to its start but travelled 8 m doing it. Always find v = 0 before answering a distance question, and state both quantities when the question asks for distance - quoting displacement for distance is a standard mark loss.

Forces and Newton's laws

Newton's second law: the resultant force on a body is F = ma (in newtons, kg and m/s^2) (Edexcel 9MA0 Topic 18; AQA 7357 R1-R3; OCR A H640 23.01/24.01). The forces to model: weight mg vertically down, the normal reaction R perpendicular to the surface, tension T along light inextensible strings, and applied forces. Draw a force diagram first in every dynamics question - it is the model, and the equations come from resolving.

Newton's third law: forces between two interacting bodies are equal, opposite and of the same type - the reason the tension is the same throughout a light string over a smooth pulley. Connected particles: write F = ma for each mass separately and solve simultaneously; the whole-system shortcut (treating the system as one mass with the external resultant force) finds the acceleration fast, but the individual equations are needed for the tension.

Worked example: connected particles over a pulley

Particles of mass 3 kg and 5 kg are connected by a light inextensible string over a smooth pulley. Find the acceleration and the tension (g = 9.8 m/s^2).

Line 1: The heavier particle moves down: for the 5 kg: 5g - T = 5a (M1: F = ma resolved).

Line 2: For the 3 kg: T - 3g = 3a (M1).

Line 3: Adding: 2g = 8a, so a = g/4 = 2.45 m/s^2 (A1).

Line 4: T = 3g + 3a = 3(9.8) + 3(2.45) = 36.75 N (A1: tension from one individual equation).

Check the tension by substituting into the other equation: 5g - 5a = 49 - 12.25 = 36.75 N - both equations agree. Modelling assumptions matter here: light (massless) string and smooth (frictionless) pulley give equal tension throughout; an extensible string would not.

Friction and inclined planes

Friction opposes relative motion and has magnitude at most F = mu R (Edexcel 9MA0 Topic 18; AQA 7357 R4-R5; OCR A H640 25.01), where mu is the coefficient of friction and R the normal reaction. Friction takes any value up to that maximum and reaches the maximum only in limiting equilibrium or when sliding - a body at rest on a shallow slope has friction exactly balancing the weight component, not necessarily mu R. Questions asking whether the body slides compare the required friction with mu R.

On an incline of angle theta, resolve parallel and perpendicular to the slope: the normal reaction is R = mg cos(theta) and the weight component along the slope is mg sin(theta). Resolving along the slope (not horizontally and vertically) is the method - diagrams with the angle marked earn the setup marks.

Worked example: sliding down a rough slope

A mass of 4 kg slides down a slope inclined at 30 degrees to the horizontal, with mu = 0.2. Find its acceleration (g = 9.8 m/s^2).

Line 1: Resolve perpendicular: R = mg cos(30 degrees) = 4(9.8)(sqrt(3)/2) = 33.9 N (M1 A1).

Line 2: Friction (opposing the downward motion): F = mu R = 0.2 x 33.9 = 6.79 N (M1 A1).

Line 3: Weight component down the slope: mg sin(30 degrees) = 4(9.8)(0.5) = 19.6 N (B1).

Line 4: Resultant: 19.6 - 6.79 = 12.8 N down the slope (M1).

Line 5: a = F/m = 12.8/4 = 3.20 m/s^2 (A1).

Common errors: using sin and cos the wrong way round (R uses cos - the reaction is perpendicular to the slope), forgetting that friction acts up the slope when the body slides down, and using F = mu R when the body is not sliding. State the direction of friction in your working - it is part of the model.

Projectiles and exam technique

A projectile under gravity alone has two independent motions: horizontal velocity constant at u cos(theta) (no horizontal force) and vertical velocity u sin(theta) with acceleration -g (Edexcel 9MA0 Topic 17; AQA 7357 Q4; OCR A H640 24.01). At maximum height the vertical velocity is zero. The three standard quantities: maximum height (from the vertical SUVAT with v = 0), time of flight (twice the time to maximum height, for level ground), and range (horizontal velocity x time of flight).

Worked example: maximum height and range

A ball is projected from ground level with speed 20 m/s at 30 degrees above the horizontal. Find the maximum height, the time of flight and the range (g = 9.8 m/s^2).

Line 1: Resolve: u_x = 20cos(30 degrees) = 17.3 m/s, u_y = 20sin(30 degrees) = 10 m/s (M1: components).

Line 2: Vertical, at max height v = 0: 0 = 10^2 - 2(9.8)s, so s = 100/19.6 = 5.10 m (M1 A1).

Line 3: Time to max height: 0 = 10 - 9.8t, so t = 1.04 s; flight time 2t = 2.04 s (A1: symmetry).

Line 4: Range = u_x x time of flight = 17.3 x 2.04 = 35.4 m (A1).

Modelling assumptions are examinable: no air resistance (so horizontal velocity is constant), the projectile is a particle (no spin or size), and gravity is uniform at 9.8 m/s^2. Questions ask which assumption is being made or what its effect would be - name it and state the consequence in context.

Exam technique across the topic: (1) draw the force diagram or resolve into components before writing equations - the diagram earns the setup marks; (2) check whether acceleration is constant (SUVAT) or variable (calculus) before selecting a method; (3) find v = 0 before any distance question; (4) state the positive direction and keep signs consistent; (5) in connected-particle questions, give the tension from an individual equation, not the whole-system equation; (6) convert units before substituting. Board coverage: Edexcel 9MA0 Topics 17-18, AQA 7357 P1-R5, OCR A H640 22.01-25.01, WJEC/Eduqas AS/A2 mechanics, CCEA AS2/A22 or AS3/A23 - identical techniques, differing wording and g conventions (9.8 or 9.81 as your board's formula booklet states).

💡 Worked Example

Exam-style: A mass of 4 kg slides down a slope inclined at 30 degrees to the horizontal. The coefficient of friction between the mass and the slope is 0.2. Find the acceleration of the mass down the slope. (g = 9.8 m/s^2) (Edexcel 9MA0-style, 7 marks)
Mark-scheme logic: Resolve perpendicular to the slope: R = mg cos(30 degrees) = 4(9.8)(sqrt(3)/2) = 33.9 N (M1 A1: normal reaction). Friction opposes the motion (up the slope) with maximum value F = mu R = 0.2 x 33.9 = 6.79 N (M1 A1: friction model). Weight component down the slope: mg sin(30 degrees) = 4(9.8)(0.5) = 19.6 N (B1). Applying Newton's second law along the slope: 19.6 - 6.79 = 4a, so the resultant is 12.8 N (M1). a = 12.8/4 = 3.20 m/s^2 down the slope (A1).

❓ Practice Questions & Mark Schemes

A particle moves with velocity v(t) = 3t^2 - 12t + 9 m/s. Find its displacement and the distance travelled from t = 0 to t = 3.
Answer: s(t) = t^3 - 6t^2 + 9t (M1 A1: integrate with s(0) = 0). Displacement: s(3) = 0 m (A1). v = 3(t - 1)(t - 3), so v = 0 at t = 1 and t = 3 (M1: direction changes). s(1) = 4, so distance = |4| + |0 - 4| = 8 m (A1: split at turning points).
Particles of mass 3 kg and 5 kg hang from a light inextensible string over a smooth pulley. Find the acceleration and the tension (g = 9.8 m/s^2).
Answer: 5 kg: 5g - T = 5a (M1). 3 kg: T - 3g = 3a (M1). Adding: 2g = 8a, so a = 2.45 m/s^2 (A1). T = 3g + 3a = 36.75 N (A1: from an individual equation). Check: 5g - 5a = 49 - 12.25 = 36.75 N agrees.
A car travelling at 25 m/s brakes uniformly and comes to rest in 50 m. Find the deceleration and the braking time.
Answer: v^2 = u^2 + 2as: 0 = 625 + 100a, so a = -6.25 m/s^2, deceleration 6.25 m/s^2 (M1 A1). v = u + at: 0 = 25 - 6.25t, so t = 4 s (A1).
A ball is projected from ground level at 20 m/s and 30 degrees above the horizontal. Find the maximum height and the range (g = 9.8 m/s^2).
Answer: u_y = 10 m/s, u_x = 17.3 m/s (M1: components). Vertical at max height: 0 = 100 - 19.6s, so s = 5.10 m (M1 A1). Time to max height 1.04 s, flight 2.04 s (A1: symmetry). Range = 17.3 x 2.04 = 35.4 m (A1).
A particle starts from rest and accelerates uniformly at 2 m/s^2 for 6 s. Find its final velocity and displacement.
Answer: v = u + at = 0 + 2(6) = 12 m/s (M1 A1). s = ut + 1/2 at^2 = 0 + 1/2 (2)(36) = 18 m (A1). Or v^2 = u^2 + 2as: 144 = 4s, s = 18 m - agreeing.
A particle moves from rest at the origin with acceleration a = 6t - 12 m/s^2. Find v(t) and s(t), and the times when it is at rest.
Answer: v(t) = 3t^2 - 12t (integral of a, v(0) = 0) (M1 A1). s(t) = t^3 - 6t^2 (integral of v, s(0) = 0) (A1). At rest: v = 3t(t - 4) = 0 at t = 0 and t = 4 s (A1).

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