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 5.5 m/s² until it stops. Find the braking distance s.
v₀ = 50 km/ha = −5.5 m/s²v = 0
s = m
2.KinematicsHard
A stone is dropped from rest into a well. The splash is heard 1.7 s after the stone is released. The speed of sound is 343 m/s; ignore air resistance and use g = 9.81 m/s². Find the depth d of the well.
ttotal = 1.7 svsound = 343 m/sg = 9.81 m/s²
d = m
3.Newton’s lawsMedium
Masses of 6 kg and 4 kg hang on either side of a light, frictionless pulley, connected by a light string. The system is released from rest. Use g = 9.81 m/s². Find the tension T in the string.
m1 = 6 kgm2 = 4 kgg = 9.81 m/s²
T = N
4.Newton’s lawsHard
A 4.5 kg block on a horizontal table is connected by a light string over a frictionless pulley to a hanging 4 kg mass. The coefficient of kinetic friction between block and table is 0.25. Use g = 9.81 m/s². Find the tension T in the string.
m1 = 4.5 kgm2 = 4 kgμ = 0.25g = 9.81 m/s²
T = N
5.Projectile motionMedium
A ball is launched from level ground at 70° above the horizontal and lands 110 m away. Ignore air resistance and use g = 9.81 m/s². Find the launch speed v0.
θ = 70°R = 110 mg = 9.81 m/s²
v0 = m/s
6.Projectile motionHard
A ball is launched at 14 m/s and 40° above the horizontal from the top of a 35 m cliff. Ignore air resistance and use g = 9.81 m/s². Find the greatest height H above the ground at the foot of the cliff.
v₀ = 14 m/sθ = 40°h = 35 mg = 9.81 m/s²
H = m
7.Circular motionMedium
A car takes a flat curve of radius 140 m. The coefficient of static friction between tyres and road is 0.3. Use g = 9.81 m/s². Find the highest speed vmax at which the car can take the curve without skidding.
r = 140 mμs = 0.3g = 9.81 m/s²
vmax = m/s
8.Circular motionHard
A 1.1 kg ball on a string 1.1 m long is swung in a vertical circle. At the lowest point it moves at 5 m/s. Use g = 9.81 m/s². Find the tension T in the string at the lowest point.
m = 1.1 kgr = 1.1 mv = 5 m/sg = 9.81 m/s²
T = N
9.Work & energyMedium
A 0.5 kg block slides 19 m down a slope at 30° to the horizontal, with a coefficient of kinetic friction of 0.1. Find the work Wf done against friction.
m = 0.5 kgθ = 30°μ = 0.1d = 19 mg = 9.81 m/s²
Wf = J
10.Work & energyHard
A 10 kg block starts from rest at the bottom of a 25° slope and is pulled up the slope by a constant force of 95 N parallel to the slope. The coefficient of kinetic friction is 0.2. Find the speed v of the block after it has moved 8 m up the slope.
A 2.5 kg glider moving at 8 m/s makes a perfectly elastic head-on collision with a 1.5 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 = 1.5 kgv1 = 8 m/sv2 = 0
v′1 = m/s
12.Momentum & collisionsHard
A 0.5 kg ball hits a wall at 24 m/s and bounces straight back at 18 m/s. The contact lasts 5 ms. Find the average force Favg of the wall on the ball.
m = 0.5 kgvin = 24 m/svout = 18 m/sΔt = 5 ms
Favg = N
13.Springs & pendulumsMedium
How long must a simple pendulum be to have a period of 0.9 s? Use g = 9.81 m/s². Find L.
T = 0.9 sg = 9.81 m/s²
L = m
14.Springs & pendulumsHard
A 2.6 kg mass on a spring with k = 470 N/m is pulled 16 cm from equilibrium and released. Find its maximum acceleration amax.
m = 2.6 kgk = 470 N/mA = 16 cm
amax = m/s²
15.Waves, sound & opticsMedium
An object stands 4 cm in front of a thin diverging lens with a focal length of 5 cm. Find the image distance di. Use the sign convention 1/f = 1/do + 1/di (f < 0 for a diverging lens, di < 0 for a virtual image).
do = 4 cmf = −5 cm
di = cm
16.Waves, sound & opticsHard
An object is 20 cm in front of a concave mirror with a radius of curvature of 20 cm. Find the magnification m (negative for an inverted image).
do = 20 cmR = 20 cm
m =
3Solutions
1.Kinematics
Answer: s = 17.54 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 = 50/3.6 = 13.89 m/s
Braking distance
0 = v₀² − 2·a·s → s = v₀²/(2a) = 13.89²/(2·5.5) = 17.54 m
Answer
s = 17.54 m
2.Kinematics
Answer: d = 13.53 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.
Two parts of the time
½·9.81·t₁² = 343·(1.7 − t₁)
4.905·t₁² + 343·t₁ − 583.1 = 0
Fall time
Only the positive root is physical.
t₁ = (−343 + √(343² + 4·4.905·583.1))/(2·4.905) = 1.661 s
Depth
d = ½·9.81·1.661² = 13.53 m
Answer
d = 13.53 m
3.Newton’s laws
Answer: T = 47.09 N
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.
Acceleration
The net driving force is the difference of the weights; it moves the total mass.
a = (6 − 4)·9.81/(6 + 4) = 1.962 m/s²
Tension from the lighter mass
T − m2·g = m2·a → T = 4·(9.81 + 1.962) = 47.09 N
Answer
T = 47.09 N
4.Newton’s laws
Answer: T = 25.97 N
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.
Solve the range formula for v₀
v₀ = √(g·R/sin 2θ) = √(9.81·110/sin 140°) = 40.97 m/s
Answer
v0 = 40.97 m/s
6.Projectile motion
Answer: H = 39.13 m
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.
Vertical launch speed
vy = 14·sin 40° = 8.999 m/s
Rise above the cliff
Δh = vy²/(2g) = 8.999²/(2·9.81) = 4.128 m
Height above the ground
H = 35 + 4.128 = 39.13 m
Answer
H = 39.13 m
7.Circular motion
Answer: vmax = 20.3 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) = √(0.3·9.81·140) = 20.3 m/s
Answer
vmax = 20.3 m/s (73.07 km/h)
8.Circular motion
Answer: T = 35.79 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 lowest point
Towards the centre (up) is positive.
T − m·g = m·v²/r
T = 1.1·9.81 + 1.1·5²/1.1 = 10.79 + 25 = 35.79 N
Answer
T = 35.79 N
9.Work & energy
Answer: Wf = 8.071 J
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).
Friction force
N = mg·cos θ = 4.905·0.866 = 4.248 N
F = μN = 0.1·4.248 = 0.4248 N
Work against friction
Wf = F·d = 0.4248·19 = 8.071 J
Answer
Wf = 8.071 J
10.Work & energy
Answer: v = 7.564 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).
Forces along the slope
m·g = 10·9.81 = 98.1 N
mg·sin θ = 41.46 N
μ·mg·cos θ = 17.78 N
Work–energy
½mv² = (95 − 59.24)·8 = 286.1 J
v = √(2·286.1/10) = 7.564 m/s
Answer
v = 7.564 m/s
11.Momentum & collisions
Answer: v′1 = 2 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 − 1.5)/(2.5 + 1.5)·8 = 2 m/s
v′2 = 2·2.5/(2.5 + 1.5)·8 = 10 m/s
Answer
v′1 = 2 m/s
12.Momentum & collisions
Answer: Favg = 4200 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 = 0.5·(18 + 24) = 21 N·s
Average force
Favg = J/Δt = 21/0.005 = 4200 N
Answer
Favg = 4200 N
13.Springs & pendulums
Answer: L = 0.2013 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·(0.9/2π)² = 0.2013 m
Answer
L = 0.2013 m
14.Springs & pendulums
Answer: amax = 28.92 m/s²
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 = √(470/2.6) = 13.45 rad/s
Maximum acceleration
amax = A·ω² = 0.16·13.45² = 28.92 m/s²
Answer
amax = 28.92 m/s²
15.Waves, sound & optics
Answer: di = −2.222 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) − 1/4
di = −2.222 cm
Ray diagram
virtual, on the same side as the object
Answer
di = −2.222 cm
16.Waves, sound & optics
Answer: m = −1
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.