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)t = ?30

A car driving at 108 km/h brakes with a constant deceleration of 6.5 m/s² until it stops. How long does braking take? Find t.

v₀ = 108 km/ha = −6.5 m/s²v = 0
t = s
2.KinematicsHard
t (s)v (m/s)6 s

A tram starts from rest and accelerates at 1.5 m/s² for 6 s, then runs at constant speed for 6 s, and finally brakes at 5 m/s² until it stops. Find the total travel time t.

a1 = 1.5 m/s²t1 = 6 st2 = 6 sa3 = −5 m/s²
t = s
3.Newton’s lawsMedium
boxv₀ = 12 m/sμ = ?

A box slides across a level floor with an initial speed of 12 m/s and comes to rest after 29 m. Use g = 9.81 m/s². Find the coefficient of kinetic friction μ.

v₀ = 12 m/sd = 29 mg = 9.81 m/s²
μ =
4.Newton’s lawsHard
m1​ = 7 kg6 kgμ = 0.25

A 7 kg block on a horizontal table is connected by a light string over a frictionless pulley to a hanging 6 kg mass. The coefficient of kinetic friction between block and table is 0.25. Use g = 9.81 m/s². Find the acceleration a of the system.

m1 = 7 kgm2 = 6 kgμ = 0.25g = 9.81 m/s²
a = m/s²
5.Projectile motionMedium
v0​ = 26 m/sθ = ?R = 40 m

A ball is launched from level ground at 26 m/s and must land 40 m away. Ignore air resistance and use g = 9.81 m/s². Find the smaller of the two possible launch angles θ.

v₀ = 26 m/sR = 40 mg = 9.81 m/s²
θ = °
6.Projectile motionHard
h = 45 mv0​ = 13 m/s20°x = ?

A ball is launched at 20° above horizontal from the top of a 45 m cliff. Ignore air resistance. Find the horizontal distance x travelled before the ball hits the ground.

v0 = 13 m/sθ = 20°h = 45 mg = 9.81 m/s²
x = m
7.Circular motionMedium
r = 90 mvmax​ = ?

A car takes a flat curve of radius 90 m. The coefficient of static friction between tyres and road is 0.6. Use g = 9.81 m/s². Find the highest speed vmax at which the car can take the curve without skidding.

r = 90 mμs = 0.6g = 9.81 m/s²
vmax = m/s
8.Circular motionHard
r = 0.6 mv = 3.5 m/s

A 0.4 kg ball on a string 0.6 m long is swung in a vertical circle. At the lowest point it moves at 3.5 m/s. Use g = 9.81 m/s². Find the tension T in the string at the lowest point.

m = 0.4 kgr = 0.6 mv = 3.5 m/sg = 9.81 m/s²
T = N
9.Work & energyMedium
45°d = 6 mμ = 0.35

A 4 kg block slides 6 m down a slope at 45° to the horizontal, with a coefficient of kinetic friction of 0.35. Find the work Wf done against friction.

m = 4 kgθ = 45°μ = 0.35d = 6 mg = 9.81 m/s²
Wf = J
10.Work & energyHard
h = 3 mL = 1 mμ = 0.3k = 2500 N/m

A 2 kg block is released from rest at height 3 m on a smooth ramp. At the bottom it crosses a rough horizontal strip 1 m long (μ = 0.3) and then runs onto a spring (k = 2500 N/m) on a smooth surface. Find the maximum compression x of the spring.

m = 2 kgh = 3 mL = 1 mμ = 0.3k = 2500 N/mg = 9.81 m/s²
x = cm
11.Momentum & collisionsMedium
1300 kg11 m/s1000 kg

A 1300 kg car moving at 11 m/s runs into a stationary 1000 kg car and the two lock together. How much kinetic energy ΔK is lost in the collision?

m1 = 1300 kgv1 = 11 m/sm2 = 1000 kgv2 = 0
ΔK = J
12.Momentum & collisionsHard
30 m/s14 m/s

A 0.45 kg ball hits a wall at 30 m/s and bounces straight back at 14 m/s. The contact lasts 5 ms. Find the average force Favg of the wall on the ball.

m = 0.45 kgvin = 30 m/svout = 14 m/sΔt = 5 ms
Favg = N
13.Springs & pendulumsMedium
L = 1 mT = 3.26 s

An astronaut on another planet finds that a simple pendulum 1 m long has a period of 3.26 s for small swings. Find the gravitational acceleration g on that planet.

L = 1 mT = 3.26 s
g = m/s²
14.Springs & pendulumsHard
2.5 kgk = 380 N/m

A 2.5 kg mass is attached to the lower end of an unstretched vertical spring with k = 380 N/m and released from rest. Use g = 9.81 m/s². Find the greatest speed vmax of the mass.

m = 2.5 kgk = 380 N/mg = 9.81 m/s²
vmax = m/s
15.Waves, sound & opticsMedium
θc = ?90°diamond, n1​ = 2.42ethanol, n2​ = 1.36

Light travels in diamond (n = 2.42) towards a flat boundary with ethanol (n = 1.36). Find the critical angle θc beyond which it is totally reflected.

n1 = 2.42n2 = 1.36
θc = °
16.Waves, sound & opticsHard
SO30 m/sf = 35 kHz

A parking sensor at rest sends ultrasound of 35 kHz towards a car that moves away at 30 m/s. Find the frequency f″ of the echo received back at the sensor (speed of sound 343 m/s).

f = 35 kHzu = 30 m/sv = 343 m/s
f″ = Hz

3Solutions

1.Kinematics

Answer: t = 4.615 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.

Units

v₀ = 108/3.6 = 30 m/s

Braking time

0 = v₀ − a·t → t = v₀/a = 30/6.5 = 4.615 s

Answer

t = 4.615 s
2.Kinematics

Answer: t = 13.8 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.

Top speed

v = a1·t1 = 1.5·6 = 9 m/s

Braking time

t3 = v/a3 = 9/5 = 1.8 s

Total time

t = 6 + 6 + 1.8 = 13.8 s

Answer

t = 13.8 s
3.Newton’s laws

Answer: μ = 0.2531

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) = 12²/(2·29) = 2.483 m/s²

Friction coefficient

μ·m·g = m·a → μ = a/g = 2.483/9.81 = 0.2531

Answer

μ = 0.2531
4.Newton’s laws

Answer: a = 3.207 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) = (58.86 − 17.17)/13 = 3.207 m/s²

Answer

a = 3.207 m/s²
5.Projectile motion

Answer: θ = 17.74 °

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.

Range formula

R = v₀²·sin 2θ/g → sin 2θ = 9.81·40/26² = 0.5805

Angle

2θ = 35.48° → θ = 17.74°

Answer

θ = 17.74°

The other solution is 90° − θ = 72.26°.

6.Projectile motion

Answer: x = 42.95 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 = 13·cos 20° = 12.22 m/s
vy = v0·sin θ = 13·sin 20° = 4.446 m/s

Time in the air

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

0 = 45 + 4.446·t − 4.905·t²
t = (vy + √(vy² + 2gh))/g = (4.446 + √(19.77 + 882.9))/9.81 = 3.516 s

Horizontal distance

x = vx·t = 12.22·3.516 = 42.95 m

Answer

x = 42.95 m
7.Circular motion

Answer: vmax = 23.02 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) = √(0.6·9.81·90) = 23.02 m/s

Answer

vmax = 23.02 m/s (82.86 km/h)
8.Circular motion

Answer: T = 12.09 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 = 0.4·9.81 + 0.4·3.5²/0.6 = 3.924 + 8.167 = 12.09 N

Answer

T = 12.09 N
9.Work & energy

Answer: Wf = 58.27 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 = 39.24·0.7071 = 27.75 N
F = μN = 0.35·27.75 = 9.711 N

Work against friction

Wf = F·d = 9.711·6 = 58.27 J

Answer

Wf = 58.27 J
10.Work & energy

Answer: x = 20.59 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 = 19.62·(3 − 0.3·1) = 52.97 J

Maximum compression

½kx² = 52.97 → x = √(2·52.97/2500) = 0.2059 m = 20.59 cm

Answer

x = 20.59 cm
11.Momentum & collisions

Answer: ΔK = 34196 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) = 1300·11/2300 = 6.217 m/s

Kinetic energy before and after

Kbefore = ½·1300·11² = 78650 J
Kafter = ½·2300·6.217² = 44454 J

Energy lost

ΔK = 78650 − 44454 = 34196 J

Answer

ΔK = 34196 J

The lost energy goes into deformation, heat and sound.

12.Momentum & collisions

Answer: Favg = 3960 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 = 0.45·(14 + 30) = 19.8 N·s

Average force

Favg = J/Δt = 19.8/0.005 = 3960 N

Answer

Favg = 3960 N
13.Springs & pendulums

Answer: g = 3.715 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.

Solve for g

g = 4π²·L/T² = 4π²·1/3.26² = 3.715 m/s²

Answer

g = 3.715 m/s²
14.Springs & pendulums

Answer: vmax = 0.7957 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 = 2.5·9.81/380 = 0.06454 m = A

Greatest speed

The speed is largest at equilibrium.

ω = √(380/2.5) = 12.33 rad/s
vmax = A·ω = 0.06454·12.33 = 0.7957 m/s

Answer

vmax = 0.7957 m/s
15.Waves, sound & optics

Answer: θc = 34.19 °

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 = 1.36/2.42 = 0.562

Critical angle

θc = arcsin(0.562) = 34.19°

Answer

θc = 34.19°
16.Waves, sound & optics

Answer: f″ = 29370 Hz

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|.

Frequency at the car

f′ = 35000·(343 − 30)/343 = 31939 Hz

Frequency of the echo

f″ = f′·343/(343 + 30) = 29370 Hz

Answer

f″ = 29370 Hz

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