Physics 1: Mechanics: cram pack

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

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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
a = ?s = 1600 m

A plane needs a speed of 240 km/h to take off and the usable runway is 1600 m long. Starting from rest, what constant acceleration a does it need?

v₀ = 0v = 240 km/hs = 1600 m
a = m/s²
2.KinematicsHard
d = ?

A stone is dropped from rest into a well. The splash is heard 4.3 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 = 4.3 svsound = 343 m/sg = 9.81 m/s²
d = m
3.Newton’s lawsMedium
boxv₀ = 7.5 m/sμ = ?

A box slides across a level floor with an initial speed of 7.5 m/s and comes to rest after 57 m. Use g = 9.81 m/s². Find the coefficient of kinetic friction μ.

v₀ = 7.5 m/sd = 57 mg = 9.81 m/s²
μ =
4.Newton’s lawsHard
m1​ = 7 kg5.5 kgno friction

A 7 kg block on a horizontal table is connected by a light string over a frictionless pulley to a hanging 5.5 kg mass. The table is frictionless. Use g = 9.81 m/s². Find the acceleration a of the system.

m1 = 7 kgm2 = 5.5 kgμ = 0g = 9.81 m/s²
a = m/s²
5.Projectile motionMedium
v0​ = ?30°R = 80 m

A ball is launched from level ground at 30° above the horizontal and lands 80 m away. Ignore air resistance and use g = 9.81 m/s². Find the launch speed v0.

θ = 30°R = 80 mg = 9.81 m/s²
v0 = m/s
6.Projectile motionHard
12 mv0​ = 32 m/s50°x = ?

A ball is thrown from ground level at 32 m/s and 50° above the horizontal. It lands on the flat roof of a building 12 m high, on its way down. Ignore air resistance and use g = 9.81 m/s². Find the horizontal distance x from the launch point to where it lands.

v₀ = 32 m/sθ = 50°hroof = 12 mg = 9.81 m/s²
x = m
7.Circular motionMedium
r = 100 m28 m/s

A 900 kg car drives over the top of a hump in the road at 28 m/s. The top of the hump is a circular arc of radius 100 m. Use g = 9.81 m/s². Find the normal force N of the road on the car at the top.

m = 900 kgv = 28 m/sr = 100 mg = 9.81 m/s²
N = N
8.Circular motionHard
r = 1.2 mv = ?

A ball on a string 1.2 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 = 1.2 mg = 9.81 m/s²
vmin = m/s
9.Work & energyMedium
30°d = 11 mμ = 0.35

A block slides from rest down a slope at 30° to the horizontal. The coefficient of kinetic friction is 0.35. Find its speed v after it has slid 11 m along the slope.

θ = 30°μ = 0.35d = 11 mg = 9.81 m/s²
v = m/s
10.Work & energyHard
h = 6 mR = 2 mv = ?

A 10 kg cart is released from rest at a height of 6 m on a smooth track that leads into a vertical circular loop of radius 2 m. Find the speed v of the cart at the top of the loop.

m = 10 kgh = 6 mR = 2 mg = 9.81 m/s²
v = m/s
11.Momentum & collisionsMedium
1000 kg24 m/s600 kg

A 1000 kg car moving at 24 m/s runs into a stationary 600 kg car and the two lock together. How much kinetic energy ΔK is lost in the collision?

m1 = 1000 kgv1 = 24 m/sm2 = 600 kgv2 = 0
ΔK = J
12.Momentum & collisionsHard
3.5 kgv = ?5 g10°L = 0.7 m

A 5 g bullet is fired horizontally into a 3.5 kg block hanging from light strings 0.7 m long, and stays in it. The strings swing out to a largest angle of 10° from the vertical. Use g = 9.81 m/s². Find the speed v of the bullet before impact.

m = 5 gM = 3.5 kgL = 0.7 mθ = 10°g = 9.81 m/s²
v = m/s
13.Springs & pendulumsMedium
L = ?

How long must a simple pendulum be to have a period of 1.4 s? Use g = 9.81 m/s². Find L.

T = 1.4 sg = 9.81 m/s²
L = m
14.Springs & pendulumsHard
1.5 kgk = 290 N/m

A 1.5 kg mass is attached to the lower end of an unstretched vertical spring with k = 290 N/m and released from rest. Use g = 9.81 m/s². Find the greatest extension xmax of the spring in cm.

m = 1.5 kgk = 290 N/mg = 9.81 m/s²
xmax = cm
15.Waves, sound & opticsMedium
θc = ?90°acrylic, n1​ = 1.49water, n2​ = 1.33

Light travels in acrylic (n = 1.49) towards a flat boundary with water (n = 1.33). Find the critical angle θc beyond which it is totally reflected.

n1 = 1.49n2 = 1.33
θc = °
16.Waves, sound & opticsHard
θn1​ = 1.46n2​ = 1.44n0​ = 1.00

An optical fibre has a core with n₁ = 1.46 and a cladding with n₂ = 1.44. Find its numerical aperture NA.

n1 = 1.46n2 = 1.44
NA =

3Solutions

1.Kinematics

Answer: a = 1.389 m/s²

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

v = 240/3.6 = 66.67 m/s

Acceleration

a = v²/(2s) = 66.67²/(2·1600) = 1.389 m/s²

Answer

a = 1.389 m/s²
2.Kinematics

Answer: d = 81 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·(4.3 − t₁)
4.905·t₁² + 343·t₁ − 1475 = 0

Fall time

Only the positive root is physical.

t₁ = (−343 + √(343² + 4·4.905·1475))/(2·4.905) = 4.064 s

Depth

d = ½·9.81·4.064² = 81 m

Answer

d = 81 m
3.Newton’s laws

Answer: μ = 0.0503

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) = 7.5²/(2·57) = 0.4934 m/s²

Friction coefficient

μ·m·g = m·a → μ = a/g = 0.4934/9.81 = 0.0503

Answer

μ = 0.0503
4.Newton’s laws

Answer: a = 4.316 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.

Acceleration of the system

a = (m2·g − μ·m1·g)/(m1 + m2) = (53.96 − 0)/12.5 = 4.316 m/s²

Answer

a = 4.316 m/s²
5.Projectile motion

Answer: v0 = 30.1 m/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.

Solve the range formula for v₀

v₀ = √(g·R/sin 2θ) = √(9.81·80/sin 60°) = 30.1 m/s

Answer

v0 = 30.1 m/s
6.Projectile motion

Answer: x = 91.48 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.

Split the launch velocity

vx = 20.57 m/s, vy = 24.51 m/s

Time to land on the roof

Larger root: the ball is descending.

12 = 24.51·t − 4.905·t²
t = (24.51 + √(24.51² − 2·9.81·12))/9.81 = 4.448 s

Horizontal distance

x = vx·t = 20.57·4.448 = 91.48 m

Answer

x = 91.48 m
7.Circular motion

Answer: N = 1773 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 = 900·9.81 − 900·28²/100 = 8829 − 7056 = 1773 N

Answer

N = 1773 N

The car feels lighter: the road pushes up less than its weight.

8.Circular motion

Answer: vmin = 3.431 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) = √(9.81·1.2) = 3.431 m/s

Answer

vmin = 3.431 m/s
9.Work & energy

Answer: v = 6.519 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 = √(2·9.81·11·(0.5 − 0.35·0.866)) = 6.519 m/s

Answer

v = 6.519 m/s
10.Work & energy

Answer: v = 6.264 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). 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·(6 − 4) = 39.24 m²/s²
v = 6.264 m/s

Answer

v = 6.264 m/s

The cart just makes it round when h = 2.5R; then N = 0 at the top.

11.Momentum & collisions

Answer: ΔK = 108000 J

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.

Common velocity

v′ = m1·v1/(m1 + m2) = 1000·24/1600 = 15 m/s

Kinetic energy before and after

Kbefore = ½·1000·24² = 288000 J
Kafter = ½·1600·15² = 180000 J

Energy lost

ΔK = 288000 − 180000 = 108000 J

Answer

ΔK = 108000 J

The lost energy goes into deformation, heat and sound.

12.Momentum & collisions

Answer: v = 320.2 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.

Rise of the block

h = L·(1 − cos θ) = 0.7·(1 − cos 10°) = 0.01063 m

Speed after impact

V = √(2·9.81·0.01063) = 0.4568 m/s

Collision

v = (m + M)·V/m = 3.505·0.4568/0.005 = 320.2 m/s

Answer

v = 320.2 m/s
13.Springs & pendulums

Answer: L = 0.487 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·(1.4/2π)² = 0.487 m

Answer

L = 0.487 m
14.Springs & pendulums

Answer: xmax = 10.15 cm

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.

Equilibrium and amplitude

x₀ = m·g/k = 1.5·9.81/290 = 0.05074 m = A

Lowest point

xmax = 2A = 0.1015 m = 10.15 cm

Answer

xmax = 10.15 cm
15.Waves, sound & optics

Answer: θc = 63.2 °

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.

Refraction at 90°

sin θc = n₂/n₁ = 1.33/1.49 = 0.8926

Critical angle

θc = arcsin(0.8926) = 63.2°

Answer

θc = 63.2°
16.Waves, sound & optics

Answer: NA = 0.2408

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.

Critical angle at the cladding

sin θc = 1.44/1.46 = 0.9863 → θc = 80.51°

Numerical aperture

NA = √(1.46² − 1.44²) = 0.2408

Answer

NA = 0.2408

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