Convert units: nm, mm and cm to m, and check whether angles are measured from the normal.
Check signs and plausibility: a virtual image has dᵢ < 0, an approaching source sounds higher, a closed pipe has only odd harmonics.
2Practice problems
1.KinematicsMedium
A car driving at 50 km/h brakes with a constant deceleration of 7.5 m/s² until it stops. How long does braking take? Find t.
v₀ = 50 km/ha = −7.5 m/s²v = 0
t = s
2.KinematicsHard
A model rocket is launched straight up from rest. Its engine gives it a constant upward acceleration of 26 m/s² for 2 s, after which the engine stops and the rocket moves freely. Ignore air resistance and use g = 9.81 m/s². Find the greatest height hmax the rocket reaches.
a = 26 m/s²t1 = 2 sg = 9.81 m/s²
hmax = m
3.Newton’s lawsMedium
A box slides across a level floor with an initial speed of 4 m/s and comes to rest after 2 m. Use g = 9.81 m/s². Find the coefficient of kinetic friction μ.
v₀ = 4 m/sd = 2 mg = 9.81 m/s²
μ =
4.Newton’s lawsHard
A 9 kg block on a horizontal table is connected by a light string over a frictionless pulley to a hanging 5 kg mass. The table is frictionless. Use g = 9.81 m/s². Find the acceleration a of the system.
m1 = 9 kgm2 = 5 kgμ = 0g = 9.81 m/s²
a = m/s²
5.Projectile motionMedium
A ball is launched at 45° above horizontal from level ground. Ignore air resistance. Find the horizontal distance x travelled before the ball hits the ground.
v0 = 14 m/sθ = 45°g = 9.81 m/s²
x = m
6.Projectile motionHard
A ball is launched at 40° above horizontal from the top of a 20 m cliff. Ignore air resistance. Find the time of flight t until the ball hits the ground.
v0 = 32 m/sθ = 40°h = 20 mg = 9.81 m/s²
t = s
7.Circular motionMedium
A car takes a flat curve of radius 70 m. The coefficient of static friction between tyres and road is 0.4. Use g = 9.81 m/s². Find the highest speed vmax at which the car can take the curve without skidding.
r = 70 mμs = 0.4g = 9.81 m/s²
vmax = m/s
8.Circular motionHard
A ball on a string 1.5 m long is swung in a vertical circle. Use g = 9.81 m/s². What is the smallest speed vmin at the top for which the string just stays tight?
r = 1.5 mg = 9.81 m/s²
vmin = m/s
9.Work & energyMedium
A 1 kg ball hangs on a light string of length 3 m. It is pulled aside until the string makes 50° with the vertical and released from rest. Find the tension T in the string when the ball passes the lowest point.
m = 1 kgL = 3 mθ = 50°g = 9.81 m/s²
T = N
10.Work & energyHard
A 0.5 kg cart is released from rest at a height of 9 m on a smooth track that leads into a vertical circular loop of radius 2 m. Find the normal force N the track exerts on the cart at the top of the loop.
m = 0.5 kgh = 9 mR = 2 mg = 9.81 m/s²
N = N
11.Momentum & collisionsMedium
A 2.5 kg glider moving at 4 m/s makes a perfectly elastic head-on collision with a 5 kg glider at rest on a frictionless track. Find the velocity v′1 of the first glider after the collision (positive in its original direction).
m1 = 2.5 kgm2 = 5 kgv1 = 4 m/sv2 = 0
v′1 = m/s
12.Momentum & collisionsHard
A 0.45 kg ball hits a wall at 25 m/s and bounces straight back at 5 m/s. The contact lasts 50 ms. Find the average force Favg of the wall on the ball.
m = 0.45 kgvin = 25 m/svout = 5 m/sΔt = 50 ms
Favg = N
13.Springs & pendulumsMedium
How long must a simple pendulum be to have a period of 2.1 s? Use g = 9.81 m/s². Find L.
T = 2.1 sg = 9.81 m/s²
L = m
14.Springs & pendulumsHard
A 2.8 kg mass on a spring with k = 80 N/m is pulled 15 cm from equilibrium and released. Find its maximum speed vmax.
m = 2.8 kgk = 80 N/mA = 15 cm
vmax = m/s
15.Waves, sound & opticsMedium
An object 3 cm tall stands 40 cm in front of a thin diverging lens with a focal length of 5 cm. Find the image height hi (negative for an inverted image).
ho = 3 cmdo = 40 cmf = −5 cm
hi = cm
16.Waves, sound & opticsHard
Light of wavelength 500 nm falls at right angles on a grating with 500 lines per millimetre. Find the angle θ2 of the order-2 maximum.
N = 500 mm⁻¹λ = 500 nmm = 2
θ2 = °
3Solutions
1.Kinematics
Answer: t = 1.852 s
Motion with constant acceleration: v = v₀ + a·t, s = v₀·t + ½·a·t² and v² = v₀² + 2·a·s. Pick the equation that contains the three things you know and the one you want, and keep the signs consistent with one positive direction.
Units
v₀ = 50/3.6 = 13.89 m/s
Braking time
0 = v₀ − a·t → t = v₀/a = 13.89/7.5 = 1.852 s
Answer
t = 1.852 s
2.Kinematics
Answer: hmax = 189.8 m
Motion with constant acceleration: v = v₀ + a·t, s = v₀·t + ½·a·t² and v² = v₀² + 2·a·s. Pick the equation that contains the three things you know and the one you want, and keep the signs consistent with one positive direction.
Powered phase
v₁ = 26·2 = 52 m/s
h₁ = ½·26·2² = 52 m
Free flight up
At the top the velocity is zero.
Δh = v₁²/(2g) = 52²/(2·9.81) = 137.8 m
hmax = 52 + 137.8 = 189.8 m
Answer
hmax = 189.8 m
3.Newton’s laws
Answer: μ = 0.4077
Newton’s second law: the net force on a body equals its mass times its acceleration, ΣF = m·a. Draw a free-body diagram, choose a positive direction along the motion, and add every force in that direction: applied forces, friction μ·N against the motion, and the components of gravity.
Deceleration
a = v₀²/(2d) = 4²/(2·2) = 4 m/s²
Friction coefficient
μ·m·g = m·a → μ = a/g = 4/9.81 = 0.4077
Answer
μ = 0.4077
4.Newton’s laws
Answer: a = 3.504 m/s²
Newton’s second law: the net force on a body equals its mass times its acceleration, ΣF = m·a. Draw a free-body diagram, choose a positive direction along the motion, and add every force in that direction: applied forces, friction μ·N against the motion, and the components of gravity.
Projectile motion: with no air resistance, x = vxt and y = h + vyt − ½gt². The two directions are independent except that they share the same time.
Split the launch velocity
Horizontal velocity stays constant; vertical motion has a constant acceleration g = 9.81 m/s² downward.
vx = v0·cos θ = 14·cos 45° = 9.899 m/s
vy = v0·sin θ = 14·sin 45° = 9.899 m/s
Time in the air
Starting and landing at the same height: t = 2vy/g.
t = 2·9.899/9.81 = 2.018 s
Horizontal distance
x = vx·t = 9.899·2.018 = 19.98 m
Answer
x = 19.98 m
6.Projectile motion
Answer: t = 5.008 s
Projectile motion: with no air resistance, x = vxt and y = h + vyt − ½gt². The two directions are independent except that they share the same time.
Split the launch velocity
Horizontal velocity stays constant; vertical motion has a constant acceleration g = 9.81 m/s² downward.
vx = v0·cos θ = 32·cos 40° = 24.51 m/s
vy = v0·sin θ = 32·sin 40° = 20.57 m/s
Time in the air
Solve y(t) = h + vy·t − ½gt² = 0 for the positive root.
0 = 20 + 20.57·t − 4.905·t²
t = (vy + √(vy² + 2gh))/g = (20.57 + √(423.1 + 392.4))/9.81 = 5.008 s
Answer
t = 5.008 s
7.Circular motion
Answer: vmax = 16.57 m/s
Uniform circular motion: an object moving at speed v on a circle of radius r accelerates towards the centre with a = v²/r, so it needs a net inward force F = m·v²/r. That force is supplied by something real: friction, tension, gravity or a normal force.
Friction provides the centripetal force
m·v²/r = μ·m·g
v = √(μ·g·r) = √(0.4·9.81·70) = 16.57 m/s
Answer
vmax = 16.57 m/s (59.66 km/h)
8.Circular motion
Answer: vmin = 3.836 m/s
Uniform circular motion: an object moving at speed v on a circle of radius r accelerates towards the centre with a = v²/r, so it needs a net inward force F = m·v²/r. That force is supplied by something real: friction, tension, gravity or a normal force.
Tension zero at the top
m·g = m·v²/r → v = √(g·r) = √(9.81·1.5) = 3.836 m/s
Answer
vmin = 3.836 m/s
9.Work & energy
Answer: T = 16.82 N
Work–energy principle: the change in kinetic energy equals the work done by all forces. Writing gravity and springs as potential energy (mgh and ½kx²) turns this into a balance: initial energy = final energy + energy lost to friction (μN·d). On a circular path the net force towards the centre must equal mv²/r.
Speed at the bottom
v² = 2gL(1 − cos θ) = 2·9.81·3·(1 − cos 50°) = 21.03 m²/s²
Forces at the bottom
m·g = 1·9.81 = 9.81 N
T = mg + mv²/L = 9.81 + 1·21.03/3 = 16.82 N
Answer
T = 16.82 N
Check: T = mg(3 − 2cos θ) = 16.82 N.
10.Work & energy
Answer: N = 19.62 N
Work–energy principle: the change in kinetic energy equals the work done by all forces. Writing gravity and springs as potential energy (mgh and ½kx²) turns this into a balance: initial energy = final energy + energy lost to friction (μN·d). On a circular path the net force towards the centre must equal mv²/r.
Speed at the top
v² = 2g(h − 2R) = 2·9.81·(9 − 4) = 98.1 m²/s²
Forces at the top
m·g = 0.5·9.81 = 4.905 N
N = mv²/R − mg = 0.5·98.1/2 − 4.905 = 19.62 N
Answer
N = 19.62 N
The cart just makes it round when h = 2.5R; then N = 0 at the top.
11.Momentum & collisions
Answer: v′1 = −1.333 m/s
Conservation of momentum: when no external force acts during a collision, the total momentum Σm·v before equals the total after. Velocities have a direction, so pick a positive direction and give velocities the other way a minus sign. In an elastic collision kinetic energy is conserved too; in a perfectly inelastic one the bodies stick together.
Elastic collision with a target at rest
Solving momentum and energy conservation together gives these two results.
v′1 = (2.5 − 5)/(2.5 + 5)·4 = −1.333 m/s
v′2 = 2·2.5/(2.5 + 5)·4 = 2.667 m/s
Answer
v′1 = −1.333 m/s
The minus sign means the first glider bounces back.
12.Momentum & collisions
Answer: Favg = 270 N
Conservation of momentum: when no external force acts during a collision, the total momentum Σm·v before equals the total after. Velocities have a direction, so pick a positive direction and give velocities the other way a minus sign. In an elastic collision kinetic energy is conserved too; in a perfectly inelastic one the bodies stick together.
Change in momentum
J = m·Δv = 0.45·(5 + 25) = 13.5 N·s
Average force
Favg = J/Δt = 13.5/0.05 = 270 N
Answer
Favg = 270 N
13.Springs & pendulums
Answer: L = 1.096 m
Simple harmonic motion: a mass m on a spring of stiffness k oscillates with angular frequency ω = √(k/m) and period T = 2π/ω = 2π·√(m/k). A simple pendulum of length L has T = 2π·√(L/g). With amplitude A, the largest speed is A·ω, the largest acceleration A·ω² and the energy ½·k·A².
Solve for the length
L = g·(T/2π)² = 9.81·(2.1/2π)² = 1.096 m
Answer
L = 1.096 m
14.Springs & pendulums
Answer: vmax = 0.8018 m/s
Simple harmonic motion: a mass m on a spring of stiffness k oscillates with angular frequency ω = √(k/m) and period T = 2π/ω = 2π·√(m/k). A simple pendulum of length L has T = 2π·√(L/g). With amplitude A, the largest speed is A·ω, the largest acceleration A·ω² and the energy ½·k·A².
Angular frequency
ω = √(80/2.8) = 5.345 rad/s
Maximum speed
vmax = A·ω = 0.15·5.345 = 0.8018 m/s
Answer
vmax = 0.8018 m/s
15.Waves, sound & optics
Answer: hi = 0.3333 cm
Geometric optics: at a boundary, n₁·sin θ₁ = n₂·sin θ₂ (Snell's law), with angles measured from the normal and n = c/v. Going into a slower medium the ray bends towards the normal. From a denser medium (n₁ > n₂) beyond the critical angle θc = arcsin(n₂/n₁) all light is reflected: total internal reflection. Thin lenses and spherical mirrors obey 1/f = 1/do + 1/di with the magnification m = −di/do. Sign convention: f > 0 for a converging lens and a concave mirror (f = R/2), f < 0 for a diverging lens and a convex mirror; di > 0 for a real image, di < 0 for a virtual one, and m < 0 for an inverted image.
Thin-lens equation
1/di = 1/f − 1/do = 1/(−5) − 1/40
di = −4.444 cm
Magnification and height
m = −(−4.444)/40 = 0.1111
hi = 0.1111·3 = 0.3333 cm
Answer
hi = 0.3333 cm
16.Waves, sound & optics
Answer: θ2 = 30 °
Interference and diffraction: light from two slits a distance d apart reaches a point on the screen with a path difference d·sin θ. Bright fringes appear where d·sin θ = mλ (m = 0, ±1, ±2, …). For a screen at distance L ≫ d, the m-th bright fringe is at y = mλL/d and the fringe spacing is Δy = λL/d. A grating with N lines per millimetre has d = 1/N and sharp maxima at d·sin θ = mλ; since sin θ ≤ 1, the highest order is the largest whole number m ≤ d/λ. A single slit of width a has dark fringes at a·sin θ = mλ, m = ±1, ±2, …