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WME02 Mechanics 2
Edexcel IAL Mathematics, M2 (A2 unit, usually Year 13). 28 lessons so far, in the suggested order.
Lessons in WME02
- Projectiles: the model and horizontal projection
Horizontal velocity is constant; vertical motion is suvat with a = 9.8 downwards. Time links the two. Combine components for the speed. - Projectiles at an angle: time of flight, range and greatest height
Vertical: 0 = (U sin α)2 - 2gH for the top, s = 0 for the landing time. Horizontal: distance = U cos α × time. Show each step when asked to derive. - Projectiles in vector form and the trajectory equation
Vector form: v = pi + (q - 9.8t)j, r = pt i + (qt - 4.9t2)j. Trajectory: y = x tan α - gx2(1 + tan2 α)/(2U2), a quadratic in tan α. - Variable acceleration: differentiating displacement
Differentiate x to get v, and v to get a. At rest: v = 0. Greatest velocity: a = 0. - Variable acceleration: integrating to find velocity and displacement
Integrate a for v, integrate v for x, and find each constant from the given conditions. A definite integral of v gives displacement. - Distance travelled when a particle changes direction
Solve v = 0, split the interval there, and add the sizes of the displacements in each part. - Differentiating position vectors
Differentiate each component. Speed is the magnitude of v. Parallel to i: j part of v is zero. - Integrating velocity and acceleration vectors
Integrate each component, add a constant vector, and use the starting velocity or position to find it. - Centre of mass of a set of particles
x̄ = Σmx/Σm and ȳ = Σmy/Σm. Treat a uniform rod as a particle at its midpoint. - Centres of mass of standard laminas and arcs
Use symmetry, then the booklet: triangle 2/3 along a median; sector 2r sin α/(3α); arc r sin α/α, with α half the angle, in radians. - Composite laminas and laminas with holes
Area acts as mass for a uniform lamina. Holes are negative areas. Tabulate area and centre of each part. - Centres of mass of wire frameworks
Wire: mass ∝ length, each piece at its midpoint (arc: r sin α/α). Lamina: mass ∝ area. - Suspended laminas and equilibrium angles
Hanging freely from P: PG is vertical. Then tan θ = perpendicular distance / distance along the edge, read from a careful sketch. - Laminas on inclined planes and hinged laminas
About to topple: the vertical through G passes through the lower corner, so tan α = (distance along) / (height of G). Hinged: moments about the hinge. - Work done, kinetic energy and potential energy
W = Fs in the direction of motion (Fs cos θ at an angle). KE = (1/2)mv2, PE = mgh: learn both. - Conservation of energy and the work-energy principle
Only gravity working: KE + PE constant. Otherwise: initial energy + work by driving forces = final energy + work against resistances. Count gravity once. - Power: driving force, maximum speed and acceleration
P = Fv, so F = P/v. Maximum speed: P/v = R. Otherwise P/v - R = ma. - Power on slopes and with towing
Uphill: P/v = R + mg sin α + ma. Downhill: P/v + mg sin α = R + ma. Towing: whole system for a, trailer alone for T. - Impulse and momentum as vectors
I = mv - mu, as vectors. Momentum is conserved component by component. Speed is the magnitude of the final velocity. - Newton's law of restitution and direct impact
CLM plus NEL (separation = e × approach), with all velocities in one positive direction. 0 ≤ e ≤ 1. - Loss of kinetic energy in collisions
Loss of KE = KE before - KE after. Impulse on one particle = its change in momentum. Zero loss only when e = 1. - Impacts with a fixed surface and bouncing
Rebound speed = e × impact speed. Impulse = mu(1 + e). Dropped from h: rebounds to e2 h. - Successive impacts
Solve each impact in turn with CLM and NEL. Another impact needs the particle behind to be moving faster towards the one in front. - Moments of forces at an angle
Moment = force × perpendicular distance = (perpendicular component) × distance along the rod. Components along the rod have no moment. - Rods hinged to a wall: reactions at a hinge
Moments about the hinge for T, then resolve horizontally and vertically for X and Y. R = sqrt(X2 + Y2). - Ladders against a smooth wall on rough ground
Smooth wall: horizontal reaction only. F = S, R = total weight, moments about the foot. About to slip: F = μR. - Rods on pegs, rough walls and limiting equilibrium
Peg reaction is perpendicular to the rod. Rough wall: normal plus friction μS. Limiting at both ends: friction = μ × reaction at both. - M2 exam technique
1 h 30 min, 75 marks, all questions. g = 9.8, answers to 2 or 3 s.f. Learn KE and PE. Follow any specified method and show all working.
Next exams for WME02
- January 2027: Wed 20 Jan 2027, afternoon, 1h 30m
- Summer 2027: Fri 4 Jun 2027, afternoon, 1h 30m
From Pearson's final timetables. All exam dates. Always confirm your entries with your exams officer.