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
t (s)v (m/s)4.167 s12.5

A car driving at 45 km/h brakes with a constant deceleration of 3 m/s² until it stops. Find the braking distance s.

v₀ = 45 km/ha = −3 m/s²v = 0
s = m
2.KinematicsHard
d = ?

A stone is dropped from rest into a well. The splash is heard 2.7 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 = 2.7 svsound = 343 m/sg = 9.81 m/s²
d = m
3.Newton’s lawsMedium
θ = 30°50 kgF = ?

A 50 kg box is pushed up a ramp at 30° to the horizontal at constant speed, by a force parallel to the ramp. The coefficient of kinetic friction is 0.2. Use g = 9.81 m/s². Find the pushing force F.

m = 50 kgθ = 30°μ = 0.2g = 9.81 m/s²
F = N
4.Newton’s lawsHard
θ = 35°blockv₀ = 10 m/s

A block is given a push so that it starts sliding up a ramp at 35° with a speed of 10 m/s. The coefficient of kinetic friction is 0.1. Use g = 9.81 m/s². How far d along the ramp does it slide before it stops?

v₀ = 10 m/sθ = 35°μ = 0.1g = 9.81 m/s²
d = m
5.Projectile motionMedium
v0​ = ?75°R = 15 m

A ball is launched from level ground at 75° above the horizontal and lands 15 m away. Ignore air resistance and use g = 9.81 m/s². Find the launch speed v0.

θ = 75°R = 15 mg = 9.81 m/s²
v0 = m/s
6.Projectile motionHard
11 mv0​ = 35 m/s70°x = ?

A ball is thrown from ground level at 35 m/s and 70° above the horizontal. It lands on the flat roof of a building 11 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 = 35 m/sθ = 70°hroof = 11 mg = 9.81 m/s²
x = m
7.Circular motionMedium
r = 110 mvmax​ = ?

A car takes a flat curve of radius 110 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 = 110 mμs = 0.3g = 9.81 m/s²
vmax = m/s
8.Circular motionHard
r = 1.2 m10 m/svtop​ = ?

A 1.8 kg ball on a light string 1.2 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 = 1.8 kgr = 1.2 mvbottom = 10 m/sg = 9.81 m/s²
Ttop = N
9.Work & energyMedium
35°d = 7 mμ = 0.1

A 5 kg block slides 7 m down a slope at 35° to the horizontal, with a coefficient of kinetic friction of 0.1. Find the work Wf done against friction.

m = 5 kgθ = 35°μ = 0.1d = 7 mg = 9.81 m/s²
Wf = J
10.Work & energyHard
k = 5000 N/m25°μ = 0.151 kg

A spring of stiffness 5000 N/m at the bottom of a 25° slope is compressed by 20 cm against a 1 kg block and released. The coefficient of kinetic friction between block and slope is 0.15. 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.)

m = 1 kgk = 5000 N/mx = 20 cmθ = 25°μ = 0.15g = 9.81 m/s²
d = m
11.Momentum & collisionsMedium
4 kgv = ?8 gh = 5 cm

An 8 g bullet is fired horizontally into a 4 kg wooden block hanging on light strings, and stays inside it. The block swings up until it is 5 cm higher than at the start. Use g = 9.81 m/s². Find the speed v of the bullet before impact.

m = 8 gM = 4 kgh = 5 cmg = 9.81 m/s²
v = m/s
12.Momentum & collisionsHard
28 m/s19 m/s

A 0.6 kg ball hits a wall at 28 m/s and bounces straight back at 19 m/s. The contact lasts 50 ms. Find the magnitude of the impulse J the wall gives the ball.

m = 0.6 kgvin = 28 m/svout = 19 m/sΔt = 50 ms
J = N·s
13.Springs & pendulumsMedium
L = ?

How long must a simple pendulum be to have a period of 1.7 s? Use g = 9.81 m/s². Find L.

T = 1.7 sg = 9.81 m/s²
L = m
14.Springs & pendulumsHard
2.1 kgk = 270 N/m

A 2.1 kg mass is attached to the lower end of an unstretched vertical spring with k = 270 N/m and released from rest. Use g = 9.81 m/s². Find the greatest speed vmax of the mass.

m = 2.1 kgk = 270 N/mg = 9.81 m/s²
vmax = m/s
15.Waves, sound & opticsMedium
FF1.5 cmdo​ = 10 cmf = −20 cm

An object 1.5 cm tall stands 10 cm in front of a thin diverging lens with a focal length of 20 cm. Find the image height hi (negative for an inverted image).

ho = 1.5 cmdo = 10 cmf = −20 cm
hi = cm
16.Waves, sound & opticsHard
Fdo​ = 5 cmR = 30 cm

An object is 5 cm in front of a concave mirror with a radius of curvature of 30 cm. Find the magnification m (negative for an inverted image).

do = 5 cmR = 30 cm
m =

3Solutions

1.Kinematics

Answer: s = 26.04 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 = 45/3.6 = 12.5 m/s

Braking distance

0 = v₀² − 2·a·s → s = v₀²/(2a) = 12.5²/(2·3) = 26.04 m

Answer

s = 26.04 m
2.Kinematics

Answer: d = 33.24 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·(2.7 − t₁)
4.905·t₁² + 343·t₁ − 926.1 = 0

Fall time

Only the positive root is physical.

t₁ = (−343 + √(343² + 4·4.905·926.1))/(2·4.905) = 2.603 s

Depth

d = ½·9.81·2.603² = 33.24 m

Answer

d = 33.24 m
3.Newton’s laws

Answer: F = 330.2 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 slope

Constant speed: the forces balance.

F = m·g·sin θ + μ·m·g·cos θ

Pushing force

F = 245.2 + 84.96 = 330.2 N

Answer

F = 330.2 N
4.Newton’s laws

Answer: d = 7.776 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 35° + 0.1·cos 35°) = 6.43 m/s²

Distance

d = v₀²/(2a) = 10²/(2·6.43) = 7.776 m

Answer

d = 7.776 m
5.Projectile motion

Answer: v0 = 17.16 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) = √(9.81·15/sin 150°) = 17.16 m/s

Answer

v0 = 17.16 m/s
6.Projectile motion

Answer: x = 76.04 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 = 11.97 m/s, vy = 32.89 m/s

Time to land on the roof

Larger root: the ball is descending.

11 = 32.89·t − 4.905·t²
t = (32.89 + √(32.89² − 2·9.81·11))/9.81 = 6.352 s

Horizontal distance

x = vx·t = 11.97·6.352 = 76.04 m

Answer

x = 76.04 m
7.Circular motion

Answer: vmax = 17.99 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) = √(0.3·9.81·110) = 17.99 m/s

Answer

vmax = 17.99 m/s (64.77 km/h)
8.Circular motion

Answer: Ttop = 61.71 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 − 4·9.81·1.2 = 52.91 m²/s²

Forces at the top

Tension and gravity both point down, towards the centre.

T + m·g = m·vtop²/r
T = 1.8·52.91/1.2 − 1.8·9.81 = 61.71 N

Answer

Ttop = 61.71 N
9.Work & energy

Answer: Wf = 28.13 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 = 49.05·0.8192 = 40.18 N
F = μN = 0.1·40.18 = 4.018 N

Work against friction

Wf = F·d = 4.018·7 = 28.13 J

Answer

Wf = 28.13 J
10.Work & energy

Answer: d = 18.25 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 = ½·5000·0.2² = 100 J

Energy balance along the slope

m·g = 1·9.81 = 9.81 N
½kx² = mg·d·(sin θ + μ·cos θ)
d = 100/(9.81·(0.4226 + 0.15·0.9063)) = 18.25 m

Answer

d = 18.25 m
11.Momentum & collisions

Answer: v = 496.2 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.

Swing after impact

V = √(2·g·h) = √(2·9.81·0.05) = 0.9905 m/s

Collision

m·v = (m + M)·V → v = (0.008 + 4)·0.9905/0.008 = 496.2 m/s

Answer

v = 496.2 m/s
12.Momentum & collisions

Answer: J = 28.2 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 = 0.6·(19 + 28) = 28.2 N·s

Answer

J = 28.2 N·s
13.Springs & pendulums

Answer: L = 0.7181 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·(1.7/2π)² = 0.7181 m

Answer

L = 0.7181 m
14.Springs & pendulums

Answer: vmax = 0.8652 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.

Equilibrium and amplitude

x₀ = m·g/k = 2.1·9.81/270 = 0.0763 m = A

Greatest speed

The speed is largest at equilibrium.

ω = √(270/2.1) = 11.34 rad/s
vmax = A·ω = 0.0763·11.34 = 0.8652 m/s

Answer

vmax = 0.8652 m/s
15.Waves, sound & optics

Answer: hi = 1 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/(−20) − 1/10
di = −6.667 cm
FF10 cmf = −20 cm

Magnification and height

m = −(−6.667)/10 = 0.6667
hi = 0.6667·1.5 = 1 cm

Answer

hi = 1 cm
16.Waves, sound & optics

Answer: m = 1.5

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.

Focal length

f = R/2 = 15 cm

Mirror equation

1/di = 1/f − 1/do = 1/15 − 1/5
di = −7.5 cm
F5 cmf = 15 cm

Magnification

m = −(−7.5)/5 = 1.5

Answer

m = 1.5

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