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 = 800 m

A plane needs a speed of 220 km/h to take off and the usable runway is 800 m long. Starting from rest, what constant acceleration a does it need?

v₀ = 0v = 220 km/hs = 800 m
a = m/s²
2.KinematicsHard
v₀ = 19 m/s35 m

A ball is thrown straight up at 19 m/s from the edge of a roof 35 m above the ground. Ignore air resistance and use g = 9.81 m/s². Find the greatest height hmax above the ground.

v₀ = 19 m/sh₀ = 35 mg = 9.81 m/s²
hmax = m
3.Newton’s lawsMedium
θ = 35°a = ?m = 17 kg

A 17 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 = 17 kgθ = 35°μ = 0.3g = 9.81 m/s²
a = m/s²
4.Newton’s lawsHard
m1​ = 3.5 kg2.5 kgθ = 20°

A 3.5 kg block on a ramp at 20° is connected by a light string over a frictionless pulley at the top of the ramp to a hanging 2.5 kg mass. The hanging mass moves down. The coefficient of kinetic friction between block and ramp is 0.25. Use g = 9.81 m/s². Find the tension T in the string.

m1 = 3.5 kgm2 = 2.5 kgθ = 20°μ = 0.25g = 9.81 m/s²
T = N
5.Projectile motionMedium
v0​ = 10 m/s70°rangeH = ?

A ball is launched at 70° above horizontal from level ground. Ignore air resistance. Find the maximum height H the ball reaches.

v0 = 10 m/sθ = 70°g = 9.81 m/s²
H = m
6.Projectile motionHard
h = 50 mv0​ = 13 m/s60°range

A ball is launched at 60° above horizontal from the top of a 50 m cliff. Ignore air resistance. Find the time of flight t until the ball hits the ground.

v0 = 13 m/sθ = 60°h = 50 mg = 9.81 m/s²
t = s
7.Circular motionMedium
θ = 15°to centrev = ?

A curve of radius 170 m is banked at 15°. At what speed v can a car take it with no friction needed at all? Use g = 9.81 m/s².

r = 170 mθ = 15°g = 9.81 m/s²
v = m/s
8.Circular motionHard
r = 0.5 mv = ?

A ball on a string 0.5 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 = 0.5 mg = 9.81 m/s²
vmin = m/s
9.Work & energyMedium
25°d = 10 mμ = 0.15

A 1 kg block slides 10 m down a slope at 25° to the horizontal, with a coefficient of kinetic friction of 0.15. Find the work Wf done against friction.

m = 1 kgθ = 25°μ = 0.15d = 10 mg = 9.81 m/s²
Wf = J
10.Work & energyHard
h = 5 mL = 1.5 mμ = 0.15k = 2000 N/m

A 2.5 kg block is released from rest at height 5 m on a smooth ramp. At the bottom it crosses a rough horizontal strip 1.5 m long (μ = 0.15) and then runs onto a spring (k = 2000 N/m) on a smooth surface. Find the maximum compression x of the spring.

m = 2.5 kgh = 5 mL = 1.5 mμ = 0.15k = 2000 N/mg = 9.81 m/s²
x = cm
11.Momentum & collisionsMedium
2000 kg17 m/s1300 kg

A 2000 kg car moving at 17 m/s runs into a stationary 1300 kg car and the two lock together. How much kinetic energy ΔK is lost in the collision?

m1 = 2000 kgv1 = 17 m/sm2 = 1300 kgv2 = 0
ΔK = J
12.Momentum & collisionsHard
18 m/s6 m/s

A 0.6 kg ball hits a wall at 18 m/s and bounces straight back at 6 m/s. The contact lasts 50 ms. Find the average force Favg of the wall on the ball.

m = 0.6 kgvin = 18 m/svout = 6 m/sΔt = 50 ms
Favg = N
13.Springs & pendulumsMedium
3.6 kgk = 310 N/mA = 15 cmx = 1 cm

A 3.6 kg mass on a spring with k = 310 N/m oscillates on a frictionless surface with an amplitude of 15 cm. Find its speed v when it is 1 cm from equilibrium.

m = 3.6 kgk = 310 N/mA = 15 cmx = 1 cm
v = m/s
14.Springs & pendulumsHard
mk = 50 N/mA = 10 cmx = 5 cm

A mass on a spring with k = 50 N/m oscillates on a frictionless surface with an amplitude of 10 cm. Find the energy U stored in the spring when the mass is 5 cm from equilibrium.

k = 50 N/mA = 10 cmx = 5 cm
U = J
15.Waves, sound & opticsMedium
L = ?n = 3

A pipe open at both ends must have its harmonic number 3 at 643 Hz. The speed of sound is 343 m/s. Find the length L of the pipe.

v = 343 m/sn = 3f3 = 643 Hz
L = m
16.Waves, sound & opticsHard
θn1​ = 1.46n2​ = 1.45n0​ = 1.00

An optical fibre has a core with n₁ = 1.46 and a cladding with n₂ = 1.45. Find its numerical aperture NA.

n1 = 1.46n2 = 1.45
NA =

3Solutions

1.Kinematics

Answer: a = 2.334 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 = 220/3.6 = 61.11 m/s

Acceleration

a = v²/(2s) = 61.11²/(2·800) = 2.334 m/s²

Answer

a = 2.334 m/s²
2.Kinematics

Answer: hmax = 53.4 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.

Rise above the roof

0 = v₀² − 2·g·Δh → Δh = 19²/(2·9.81) = 18.4 m

Height above the ground

hmax = 35 + 18.4 = 53.4 m

Answer

hmax = 53.4 m
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: T = 22.56 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.

Forces along the string

m₂·g = 24.53 N
m₁·g·sin θ = 11.74 N
μ·m₁·g·cos θ = 8.066 N

Acceleration of the system

a = (24.53 − 11.74 − 8.066)/6 = 0.7859 m/s²

Tension from the hanging mass

m2·g − T = m2·a → T = 2.5·(9.81 − 0.7859) = 22.56 N

Answer

T = 22.56 N
5.Projectile motion

Answer: H = 4.501 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

Horizontal velocity stays constant; vertical motion has a constant acceleration g = 9.81 m/s² downward.

vx = v0·cos θ = 10·cos 70° = 3.42 m/s
vy = v0·sin θ = 10·sin 70° = 9.397 m/s

Highest point

At the top the vertical velocity is zero: vy² = 2gH.

H = vy²/(2g) = 9.397²/(2·9.81) = 4.501 m

Answer

H = 4.501 m
6.Projectile motion

Answer: t = 4.54 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 = 13·cos 60° = 6.5 m/s
vy = v0·sin θ = 13·sin 60° = 11.26 m/s

Time in the air

Solve y(t) = h + vy·t − ½gt² = 0 for the positive root.

0 = 50 + 11.26·t − 4.905·t²
t = (vy + √(vy² + 2gh))/g = (11.26 + √(126.7 + 981))/9.81 = 4.54 s

Answer

t = 4.54 s
7.Circular motion

Answer: v = 21.14 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 balance

N·cos θ = m·g, N·sin θ = m·v²/r → tan θ = v²/(r·g)

Speed

v = √(r·g·tan θ) = √(170·9.81·tan 15°) = 21.14 m/s

Answer

v = 21.14 m/s
(76.1 km/h)
8.Circular motion

Answer: vmin = 2.215 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) = √(9.81·0.5) = 2.215 m/s

Answer

vmin = 2.215 m/s
9.Work & energy

Answer: Wf = 13.34 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 = 9.81·0.9063 = 8.891 N
F = μN = 0.15·8.891 = 1.334 N

Work against friction

Wf = F·d = 1.334·10 = 13.34 J

Answer

Wf = 13.34 J
10.Work & energy

Answer: x = 34.22 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·(5 − 0.15·1.5) = 117.1 J

Maximum compression

½kx² = 117.1 → x = √(2·117.1/2000) = 0.3422 m = 34.22 cm

Answer

x = 34.22 cm
11.Momentum & collisions

Answer: ΔK = 113848 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) = 2000·17/3300 = 10.3 m/s

Kinetic energy before and after

Kbefore = ½·2000·17² = 289000 J
Kafter = ½·3300·10.3² = 175152 J

Energy lost

ΔK = 289000 − 175152 = 113848 J

Answer

ΔK = 113848 J

The lost energy goes into deformation, heat and sound.

12.Momentum & collisions

Answer: Favg = 288 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 = 0.6·(6 + 18) = 14.4 N·s

Average force

Favg = J/Δt = 14.4/0.05 = 288 N

Answer

Favg = 288 N
13.Springs & pendulums

Answer: v = 1.389 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 = √(310/3.6) = 9.28 rad/s

Speed at x

v = ω·√(A² − x²) = 9.28·√(0.15² − 0.01²) = 1.389 m/s

Answer

v = 1.389 m/s
14.Springs & pendulums

Answer: U = 0.0625 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 = ½·50·0.1² = 0.25 J

Spring energy at x

U = ½·k·x² = ½·50·0.05² = 0.0625 J

Answer

U = 0.0625 J
15.Waves, sound & optics

Answer: L = 0.8002 m

Standing waves and the Doppler effect: a string fixed at both ends, or a pipe open at both ends, fits whole half-wavelengths: L = nλ/2, fn = n·v/(2L), n = 1, 2, 3, … A pipe closed at one end has a node at the closed end and an antinode at the open end: L = nλ/4 with odd n only, fn = n·v/(4L). When source or observer move along the line between them, f′ = f·(v ± vo)/(v ∓ vs): use the upper signs for motion towards each other. Two waves of nearly equal frequency beat at |f₁ − f₂|.

Wavelength

λ = v/f = 343/643 = 0.5334 m

Length

L = nλ/2 = 3·0.5334/2 = 0.8002 m

Answer

L = 0.8002 m
16.Waves, sound & optics

Answer: NA = 0.1706

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 = 1.45/1.46 = 0.9932 → θc = 83.29°

Numerical aperture

NA = √(1.46² − 1.45²) = 0.1706

Answer

NA = 0.1706

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