Physics 1: Mechanics: cram pack

Formula sheets, the key method steps for every topic and 16 practice problems, with full solutions at the back.

New problemsBack to the course

In the print window, choose “Save as PDF” to keep a copy on your device.

1Formulas and methods

Kinematics

Velocity
v = v0 + a·t
Displacement
s = v0·t + ½·a·t²
Without time
v² = v0² + 2·a·s
Units
1 m/s = 3.6 km/h

Method

  1. List what you know: v₀, v, a, t and s, with units.
  2. Pick the equation that contains your three knowns and the unknown.
  3. Choose one positive direction and give opposing quantities a minus sign.
  4. Solve and check that the answer is physically sensible.

Newton’s laws

Second law
ΣF = m·a
Weight
W = m·g
Kinetic friction
Ff = μ·N
On a slope
along: m·g·sin θ, normal: m·g·cos θ

Method

  1. Draw a free-body diagram with every force on the body.
  2. Choose a positive direction along the motion.
  3. Split forces into components along and perpendicular to the motion (on a slope: m·g·sin θ along, m·g·cos θ into the slope).
  4. Apply ΣF = m·a along the motion; friction is μ·N against the motion.

Projectile motion

Components
vx = v0cos θ, vy = v0sin θ
Position
x = vxt, y = h + vyt − ½gt²
Maximum height
H = h + vy²/(2g)
Range (level ground)
R = v0²·sin 2θ/g

Method

  1. Split the launch velocity into components: vx = v₀·cos θ and vy = v₀·sin θ.
  2. The horizontal motion has constant speed; the vertical motion has acceleration −g.
  3. Find the time of flight from the vertical motion.
  4. Use that time in the horizontal motion to find the range.

Circular motion

Centripetal acceleration
a = v²/r = ω²·r
Centripetal force
F = m·v²/r
Angular speed
ω = v/r = 2π/T
Flat curve, friction
vmax = √(μ·g·r)

Work & energy

Kinetic energy
Ek = ½mv²
Potential energy
Ep = mgh
Energy balance
Ek1 + Ep1 + W = Ek2 + Ep2 + losses
Work of friction
W = μ·N·d
Power
P = W/t

Momentum & collisions

Momentum
p = m·v
Conservation
Σm·v (before) = Σm·v (after)
Perfectly inelastic
v′ = (m1v1 + m2v2)/(m1 + m2)
Impulse
J = F·Δt = m·Δv

Method

  1. Choose a positive direction and give each velocity its sign.
  2. Write the total momentum before: Σm·v.
  3. For a perfectly inelastic collision the bodies move together after; for an elastic one kinetic energy is also conserved.
  4. Set momentum before equal to momentum after and solve.

Springs & pendulums

Mass on a spring
T = 2π·√(m/k)
Pendulum
T = 2π·√(L/g)
Angular frequency
ω = √(k/m) = 2π/T
Maximum speed and acceleration
vmax = A·ω, amax = A·ω²
Energy
E = ½·k·A²

Waves, sound & optics

Wave speed
v = fλ, T = 1/f
String
v = √(T/μ), μ = m/L
Sound level
β = 10·log10(I/I0), I0 = 10⁻¹² W/m²
Point source
I = P/(4πr²)
Standing waves
string or open pipe fn = n·v/(2L); closed pipe fn = n·v/(4L), n odd
Doppler effect
f′ = f·(v ± vo)/(v ∓ vs)
Refractive index
n = c/v, λ = λ0/n
Snell’s law
n1sin θ1 = n2sin θ2
Critical angle
sin θc = n2/n1
Optical fibre
NA = sin θa = √(n1² − n2²)
Lenses and mirrors
1/f = 1/do + 1/di, m = −di/do, mirror f = R/2
Double slit
d·sin θ = mλ, ym = mλL/d
Grating
d = 1/N, d·sin θ = mλ, mmax ≤ d/λ
Single slit
a·sin θ = mλ (dark), w = 2λL/a

Method

  1. Identify the kind of problem: wave speed, sound level, standing wave, Doppler, refraction, lens or mirror, or interference.
  2. Write the relation first: v = fλ, β = 10·log(I/I₀), fₙ = n·v/(2L) or n·v/(4L), f′ = f(v ± vo)/(v ∓ vs), n₁sin θ₁ = n₂sin θ₂, 1/f = 1/d₀ + 1/dᵢ, d·sin θ = mλ.
  3. Convert units: nm, mm and cm to m, and check whether angles are measured from the normal.
  4. 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
t (s)v (m/s)6.25 s25

A car driving at 90 km/h brakes with a constant deceleration of 4 m/s² until it stops. Find the braking distance s.

v₀ = 90 km/ha = −4 m/s²v = 0
s = m
2.KinematicsHard
v₀ = 8 m/s30 m

A ball is thrown straight up at 8 m/s from the edge of a roof 30 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 = 8 m/sh₀ = 30 mg = 9.81 m/s²
t = s
3.Newton’s lawsMedium
θ = 35°a = ?m = 4 kg

A 4 kg block slides down a slope at 35° to the horizontal. The coefficient of kinetic friction is 0.3. Use g = 9.81 m/s². Find the acceleration a of the block along the slope.

m = 4 kgθ = 35°μ = 0.3g = 9.81 m/s²
a = m/s²
4.Newton’s lawsHard
θ = 30°blockv₀ = 9 m/s

A block is given a push so that it starts sliding up a ramp at 30° with a speed of 9 m/s. The coefficient of kinetic friction is 0.25. Use g = 9.81 m/s². How far d along the ramp does it slide before it stops?

v₀ = 9 m/sθ = 30°μ = 0.25g = 9.81 m/s²
d = m
5.Projectile motionMedium
45 my = ?v0​ = 28 m/s35°

A ball is kicked from level ground at 28 m/s and 35° above the horizontal towards a wall 45 m away. Ignore air resistance and use g = 9.81 m/s². At what height y does the ball pass the wall?

v₀ = 28 m/sθ = 35°x = 45 mg = 9.81 m/s²
y = m
6.Projectile motionHard
h = 55 mv0​ = 11 m/s45°H = ?

A ball is launched at 11 m/s and 45° above the horizontal from the top of a 55 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 = 11 m/sθ = 45°h = 55 mg = 9.81 m/s²
H = m
7.Circular motionMedium
r = 140 mvmax​ = ?

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
θ = 20°to centrevmin​ = ?

A curve of radius 100 m is banked at 20°, and the coefficient of static friction between tyres and road is 0.3. Use g = 9.81 m/s². Find the lowest speed vmin at which a car can take the curve without sliding down the bank.

r = 100 mθ = 20°μs = 0.3g = 9.81 m/s²
vmin = m/s
9.Work & energyMedium
35°d = 8 mμ = 0.35

A 2.5 kg block slides 8 m down a slope at 35° to the horizontal, with a coefficient of kinetic friction of 0.35. Find the work Wf done against friction.

m = 2.5 kgθ = 35°μ = 0.35d = 8 mg = 9.81 m/s²
Wf = J
10.Work & energyHard
h = 2.5 mL = 1.5 mμ = 0.1k = 2500 N/m

A 2.5 kg block is released from rest at height 2.5 m on a smooth ramp. At the bottom it crosses a rough horizontal strip 1.5 m long (μ = 0.1) and then runs onto a spring (k = 2500 N/m) on a smooth surface. Find the maximum compression x of the spring.

m = 2.5 kgh = 2.5 mL = 1.5 mμ = 0.1k = 2500 N/mg = 9.81 m/s²
x = cm
11.Momentum & collisionsMedium
4.5 kg3 m/s2.5 kg

A 4.5 kg glider moving at 3 m/s makes a perfectly elastic head-on collision with a 2.5 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 = 4.5 kgm2 = 2.5 kgv1 = 3 m/sv2 = 0
v′1 = m/s
12.Momentum & collisionsHard
18 m/s8 m/s

A 0.1 kg ball hits a wall at 18 m/s and bounces straight back at 8 m/s. The contact lasts 5 ms. Find the magnitude of the impulse J the wall gives the ball.

m = 0.1 kgvin = 18 m/svout = 8 m/sΔt = 5 ms
J = N·s
13.Springs & pendulumsMedium
L = ?

How long must a simple pendulum be to have a period of 1.9 s? Use g = 9.81 m/s². Find L.

T = 1.9 sg = 9.81 m/s²
L = m
14.Springs & pendulumsHard
1.6 kgk = 130 N/mA = 3 cm

A 1.6 kg mass on a spring with k = 130 N/m is pulled 3 cm from equilibrium and released. Find its maximum acceleration amax.

m = 1.6 kgk = 130 N/mA = 3 cm
amax = m/s²
15.Waves, sound & opticsMedium
FFdo​ = 15 cmf = 10 cm

An object stands 15 cm in front of a thin converging lens with a focal length of 10 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 = 15 cmf = 10 cm
di = cm
16.Waves, sound & opticsHard
λ = 600 nma = 0.05 mm

Light of wavelength 600 nm passes through a single slit 0.05 mm wide. Find the angle θ1 of dark fringe number 1 from the straight-through direction.

λ = 600 nma = 0.05 mmm = 1
θ1 = °

3Solutions

1.Kinematics

Answer: s = 78.13 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 = 90/3.6 = 25 m/s

Braking distance

0 = v₀² − 2·a·s → s = v₀²/(2a) = 25²/(2·4) = 78.13 m

Answer

s = 78.13 m
2.Kinematics

Answer: t = 3.42 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.

−30 = 8·t − ½·9.81·t²
4.905·t² − 8·t − 30 = 0

Solve the quadratic

Only the positive root is physical.

t = (8 + √(8² + 2·9.81·30))/9.81 = 3.42 s

Answer

t = 3.42 s
3.Newton’s laws

Answer: a = 3.216 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.

Forces along the slope

Down the slope is positive.

m·a = m·g·sin θ − μ·m·g·cos θ

Acceleration

a = 9.81·(sin 35° − 0.3·cos 35°) = 9.81·(0.5736 − 0.2457) = 3.216 m/s²

Answer

a = 3.216 m/s²
4.Newton’s laws

Answer: d = 5.762 m

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

Both forces point down the slope; the mass cancels.

a = 9.81·(sin 30° + 0.25·cos 30°) = 7.029 m/s²

Distance

d = v₀²/(2a) = 9²/(2·7.029) = 5.762 m

Answer

d = 5.762 m
5.Projectile motion

Answer: y = 12.63 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.

Time to the wall

vx = 28·cos 35° = 22.94 m/s
t = x/vx = 45/22.94 = 1.962 s

Height at that time

y = 16.06·1.962 − ½·9.81·1.962² = 12.63 m

Answer

y = 12.63 m

The ball is already on its way down at the wall.

6.Projectile motion

Answer: H = 58.08 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 = 11·sin 45° = 7.778 m/s

Rise above the cliff

Δh = vy²/(2g) = 7.778²/(2·9.81) = 3.084 m

Height above the ground

H = 55 + 3.084 = 58.08 m

Answer

H = 58.08 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: vmin = 7.522 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.

Force balances

Friction points up the slope.

N·(sin θ − μ·cos θ) = m·v²/r
N·(cos θ + μ·sin θ) = m·g

Speed

v = √(100·9.81·0.06011/1.042) = 7.522 m/s

Answer

vmin = 7.522 m/s
(27.08 km/h)
9.Work & energy

Answer: Wf = 56.25 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 = 24.53·0.8192 = 20.09 N
F = μN = 0.35·20.09 = 7.031 N

Work against friction

Wf = F·d = 7.031·8 = 56.25 J

Answer

Wf = 56.25 J
10.Work & energy

Answer: x = 21.47 cm

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 left after the rough strip

The ramp is smooth, so only the strip removes energy.

mgh − μmgL = 24.53·(2.5 − 0.1·1.5) = 57.63 J

Maximum compression

½kx² = 57.63 → x = √(2·57.63/2500) = 0.2147 m = 21.47 cm

Answer

x = 21.47 cm
11.Momentum & collisions

Answer: v′1 = 0.8571 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 = (4.5 − 2.5)/(4.5 + 2.5)·3 = 0.8571 m/s
v′2 = 2·4.5/(4.5 + 2.5)·3 = 3.857 m/s

Answer

v′1 = 0.8571 m/s
12.Momentum & collisions

Answer: J = 2.6 N·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.

Change in momentum

J = m·Δv = 0.1·(8 + 18) = 2.6 N·s

Answer

J = 2.6 N·s
13.Springs & pendulums

Answer: L = 0.897 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·(1.9/2π)² = 0.897 m

Answer

L = 0.897 m
14.Springs & pendulums

Answer: amax = 2.437 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 = √(130/1.6) = 9.014 rad/s

Maximum acceleration

amax = A·ω² = 0.03·9.014² = 2.437 m/s²

Answer

amax = 2.437 m/s²
15.Waves, sound & optics

Answer: di = 30 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 = 1/10 − 1/15
di = 30 cm
FF15 cmf = 10 cm

Ray diagram

real, on the far side of the lens

Answer

di = 30 cm
16.Waves, sound & optics

Answer: θ1 = 0.6876 °

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, …

Dark fringe condition

sin θ = mλ/a = 0.012
θ = 0.6876°

Answer

θ1 = 0.6876°

ExamProblems · examproblems.com/courses/physics-1-mechanics