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 driver moving at 54 km/h sees an obstacle. Her reaction time is 1.2 s, after which the car brakes with a constant deceleration of 7.5 m/s². Find the total stopping distance d from the moment she sees the obstacle.
v₀ = 54 km/htr = 1.2 sa = −7.5 m/s²
d = m
2.KinematicsHard
A ball is thrown straight up at 7 m/s from the edge of a roof 5 m above the ground. Ignore air resistance and use g = 9.81 m/s². How long after the throw does it hit the ground? Find t.
v₀ = 7 m/sh₀ = 5 mg = 9.81 m/s²
t = s
3.Newton’s lawsMedium
A 19 kg block slides down a slope at 20° to the horizontal. The coefficient of kinetic friction is 0.2. Use g = 9.81 m/s². Find the acceleration a of the block along the slope.
m = 19 kgθ = 20°μ = 0.2g = 9.81 m/s²
a = m/s²
4.Newton’s lawsHard
Two blocks on a level floor are joined by a light horizontal string. A horizontal force of 45 N pulls the front 11 kg block; the 7 kg block is towed behind. The coefficient of kinetic friction is 0.1 for both blocks. Use g = 9.81 m/s². Find the acceleration a of the blocks.
m1 = 7 kgm2 = 11 kgF = 45 Nμ = 0.1g = 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 = 30 m/sθ = 45°g = 9.81 m/s²
x = m
6.Projectile motionHard
A ball is launched at 12 m/s and 35° above the horizontal from the top of a 50 m cliff. Ignore air resistance and use g = 9.81 m/s². At what angle α below the horizontal does it hit the ground?
v₀ = 12 m/sθ = 35°h = 50 mg = 9.81 m/s²
α = °
7.Circular motionMedium
A 1300 kg car drives over the top of a hump in the road at 6 m/s. The top of the hump is a circular arc of radius 30 m. Use g = 9.81 m/s². Find the normal force N of the road on the car at the top.
m = 1300 kgv = 6 m/sr = 30 mg = 9.81 m/s²
N = N
8.Circular motionHard
A 1 kg ball on a light string 0.8 m long is swung in a vertical circle. At the lowest point its speed is 10 m/s. Ignore air resistance and use g = 9.81 m/s². Find the tension Ttop in the string at the highest point.
m = 1 kgr = 0.8 mvbottom = 10 m/sg = 9.81 m/s²
Ttop = N
9.Work & energyMedium
A block slides from rest down a slope at 20° to the horizontal. The coefficient of kinetic friction is 0.2. Find its speed v after it has slid 6 m along the slope.
θ = 20°μ = 0.2d = 6 mg = 9.81 m/s²
v = m/s
10.Work & energyHard
A spring of stiffness 800 N/m at the bottom of a 30° slope is compressed by 20 cm against a 0.5 kg block and released. The coefficient of kinetic friction between block and slope is 0.3. How far d up the slope does the block travel from the release point before it stops? (Ignore the short distance over which the spring pushes, i.e. take friction and gravity over the whole distance d.)
A 5 g bullet is fired horizontally into a 2 kg wooden block hanging on light strings, and stays inside it. The block swings up until it is 7 cm higher than at the start. Use g = 9.81 m/s². Find the speed v of the bullet before impact.
m = 5 gM = 2 kgh = 7 cmg = 9.81 m/s²
v = m/s
12.Momentum & collisionsHard
A 5 g bullet is fired horizontally into a 1.5 kg block hanging from light strings 1.5 m long, and stays in it. The strings swing out to a largest angle of 15° from the vertical. Use g = 9.81 m/s². Find the speed v of the bullet before impact.
m = 5 gM = 1.5 kgL = 1.5 mθ = 15°g = 9.81 m/s²
v = m/s
13.Springs & pendulumsMedium
A 3.1 kg mass on a spring with k = 340 N/m is pulled 7 cm in the positive direction and released from rest at t = 0. Find its velocity v at t = 0.8 s (with sign).
m = 3.1 kgk = 340 N/mA = 7 cmt = 0.8 s
v = m/s
14.Springs & pendulumsHard
A mass on a spring with k = 140 N/m oscillates on a frictionless surface with an amplitude of 6 cm. Find the energy U stored in the spring when the mass is 3 cm from equilibrium.
k = 140 N/mA = 6 cmx = 3 cm
U = J
15.Waves, sound & opticsMedium
An object 4 cm tall stands 50 cm in front of a thin converging lens with a focal length of 12 cm. Find the image height hi (negative for an inverted image).
ho = 4 cmdo = 50 cmf = 12 cm
hi = cm
16.Waves, sound & opticsHard
Light of wavelength 450 nm falls at right angles on a grating with 500 lines per millimetre. Find the angle θ3 of the order-3 maximum.
N = 500 mm⁻¹λ = 450 nmm = 3
θ3 = °
3Solutions
1.Kinematics
Answer: d = 33 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.
Units
v₀ = 54/3.6 = 15 m/s
Reaction distance
d1 = v₀·tr = 15·1.2 = 18 m
Braking distance
d2 = v₀²/(2a) = 15²/(2·7.5) = 15 m
Total
d = 18 + 15 = 33 m
Answer
d = 33 m
2.Kinematics
Answer: t = 1.95 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.
Equation of motion
Up is positive and the ground is h₀ below the starting point.
−5 = 7·t − ½·9.81·t²
4.905·t² − 7·t − 5 = 0
Solve the quadratic
Only the positive root is physical.
t = (7 + √(7² + 2·9.81·5))/9.81 = 1.95 s
Answer
t = 1.95 s
3.Newton’s laws
Answer: a = 1.512 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.
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 = 30·cos 45° = 21.21 m/s
vy = v0·sin θ = 30·sin 45° = 21.21 m/s
Time in the air
Starting and landing at the same height: t = 2vy/g.
t = 2·21.21/9.81 = 4.325 s
Horizontal distance
x = vx·t = 21.21·4.325 = 91.74 m
Answer
x = 91.74 m
6.Projectile motion
Answer: α = 72.96 °
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
vx = 12·cos 35° = 9.83 m/s
vy0 = 12·sin 35° = 6.883 m/s
Vertical speed at impact
Energy or v² = v₀² + 2as in the vertical direction.
vy = √(6.883² + 2·9.81·50) = 32.07 m/s
Impact angle
tan α = vy/vx = 32.07/9.83 → α = 72.96°
Answer
α = 72.96°
7.Circular motion
Answer: N = 11193 N
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.
Forces at the top
Towards the centre (down) is positive.
m·g − N = m·v²/r
N = 1300·9.81 − 1300·6²/30 = 12753 − 1560 = 11193 N
Answer
N = 11193 N
The car feels lighter: the road pushes up less than its weight.
8.Circular motion
Answer: Ttop = 75.95 N
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.
Speed at the top
Kinetic energy is traded for potential energy over a height 2r.
vtop² = 10² − 4·9.81·0.8 = 68.61 m²/s²
Forces at the top
Tension and gravity both point down, towards the centre.
T + m·g = m·vtop²/r
T = 1·68.61/0.8 − 1·9.81 = 75.95 N
Answer
Ttop = 75.95 N
9.Work & energy
Answer: v = 4.259 m/s
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).
Energy balance along the slope
The block drops a height d·sin θ while friction removes μmg·cos θ·d. The mass cancels.
½v² = g·d·(sin θ − μ·cos θ)
v = √(2·9.81·6·(0.342 − 0.2·0.9397)) = 4.259 m/s
Answer
v = 4.259 m/s
10.Work & energy
Answer: d = 4.293 m
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).
Spring energy
x = 20 cm = 0.2 m
½kx² = ½·800·0.2² = 16 J
Energy balance along the slope
m·g = 0.5·9.81 = 4.905 N
½kx² = mg·d·(sin θ + μ·cos θ)
d = 16/(4.905·(0.5 + 0.3·0.866)) = 4.293 m
Answer
d = 4.293 m
11.Momentum & collisions
Answer: v = 469.9 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.
Swing after impact
V = √(2·g·h) = √(2·9.81·0.07) = 1.172 m/s
Collision
m·v = (m + M)·V → v = (0.005 + 2)·1.172/0.005 = 469.9 m/s
Answer
v = 469.9 m/s
12.Momentum & collisions
Answer: v = 301.4 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.
Rise of the block
h = L·(1 − cos θ) = 1.5·(1 − cos 15°) = 0.05111 m
Speed after impact
V = √(2·9.81·0.05111) = 1.001 m/s
Collision
v = (m + M)·V/m = 1.505·1.001/0.005 = 301.4 m/s
Answer
v = 301.4 m/s
13.Springs & pendulums
Answer: v = −0.6347 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 = √(340/3.1) = 10.47 rad/s
ω·t = 10.47·0.8 = 8.378 rad
Velocity
v = −A·ω·sin(ω·t) = −0.07·10.47·sin(8.378) = −0.6347 m/s
Answer
v = −0.6347 m/s
14.Springs & pendulums
Answer: U = 0.063 J
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.
Total energy
E = ½·k·A² = ½·140·0.06² = 0.252 J
Spring energy at x
U = ½·k·x² = ½·140·0.03² = 0.063 J
Answer
U = 0.063 J
15.Waves, sound & optics
Answer: hi = −1.263 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 = 1/12 − 1/50
di = 15.79 cm
Magnification and height
m = −15.79/50 = −0.3158
hi = −0.3158·4 = −1.263 cm
Answer
hi = −1.263 cm
16.Waves, sound & optics
Answer: θ3 = 42.45 °
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, …