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)1.818 s10

A car driving at 36 km/h brakes with a constant deceleration of 5.5 m/s² until it stops. Find the braking distance s.

v₀ = 36 km/ha = −5.5 m/s²v = 0
s = m
2.KinematicsHard
AB: 23 m/s20 m

Ball A is dropped from rest from a height of 20 m. At the same instant ball B is thrown straight up from the ground directly below at 23 m/s. Ignore air resistance and use g = 9.81 m/s². At what height y above the ground do they meet?

H = 20 mv0B = 23 m/sg = 9.81 m/s²
y = m
3.Newton’s lawsMedium
40 kg25°F = 200 Nμ = 0.4

A 40 kg sled is pulled across level snow by a rope at 25° above the horizontal with a force of 200 N. The coefficient of kinetic friction is 0.4. Use g = 9.81 m/s². Find the acceleration a of the sled.

m = 40 kgF = 200 Nθ = 25°μ = 0.4g = 9.81 m/s²
a = m/s²
4.Newton’s lawsHard
m1​ = 3 kg5 kgμ = 0.1

A 3 kg block on a horizontal table is connected by a light string over a frictionless pulley to a hanging 5 kg mass. The coefficient of kinetic friction between block and table is 0.1. Use g = 9.81 m/s². Find the acceleration a of the system.

m1 = 3 kgm2 = 5 kgμ = 0.1g = 9.81 m/s²
a = m/s²
5.Projectile motionMedium
v0​ = 36 m/sθ = ?R = 110 m

A ball is launched from level ground at 36 m/s and must land 110 m away. Ignore air resistance and use g = 9.81 m/s². Find the smaller of the two possible launch angles θ.

v₀ = 36 m/sR = 110 mg = 9.81 m/s²
θ = °
6.Projectile motionHard
27 mv0​ = 39 m/s55°x = ?

A ball is thrown from ground level at 39 m/s and 55° above the horizontal. It lands on the flat roof of a building 27 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 = 39 m/sθ = 55°hroof = 27 mg = 9.81 m/s²
x = m
7.Circular motionMedium
r = 55 mvmax​ = ?

A car takes a flat curve of radius 55 m. The coefficient of static friction between tyres and road is 0.8. Use g = 9.81 m/s². Find the highest speed vmax at which the car can take the curve without skidding.

r = 55 mμs = 0.8g = 9.81 m/s²
vmax = m/s
8.Circular motionHard
r = 0.7 mv = 7.5 m/s

A 1.7 kg ball on a string 0.7 m long is swung in a vertical circle. At the lowest point it moves at 7.5 m/s. Use g = 9.81 m/s². Find the tension T in the string at the lowest point.

m = 1.7 kgr = 0.7 mv = 7.5 m/sg = 9.81 m/s²
T = N
9.Work & energyMedium
30°d = 6 mμ = 0.15

A block slides from rest down a slope at 30° to the horizontal. The coefficient of kinetic friction is 0.15. Find its speed v after it has slid 6 m along the slope.

θ = 30°μ = 0.15d = 6 mg = 9.81 m/s²
v = m/s
10.Work & energyHard
h = 3 mL = 1.5 mμ = 0.2k = 2000 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 1.5 m long (μ = 0.2) and then runs onto a spring (k = 2000 N/m) on a smooth surface. Find the speed v of the block when it reaches the spring.

m = 2 kgh = 3 mL = 1.5 mμ = 0.2k = 2000 N/mg = 9.81 m/s²
v = m/s
11.Momentum & collisionsMedium
1.5 kgv = ?8 gh = 11 cm

An 8 g bullet is fired horizontally into a 1.5 kg wooden block hanging on light strings, and stays inside it. The block swings up until it is 11 cm higher than at the start. Use g = 9.81 m/s². Find the speed v of the bullet before impact.

m = 8 gM = 1.5 kgh = 11 cmg = 9.81 m/s²
v = m/s
12.Momentum & collisionsHard
21 m/s12 m/s

A 0.1 kg ball hits a wall at 21 m/s and bounces straight back at 12 m/s. The contact lasts 25 ms. Find the magnitude of the impulse J the wall gives the ball.

m = 0.1 kgvin = 21 m/svout = 12 m/sΔt = 25 ms
J = N·s
13.Springs & pendulumsMedium
L = ?

How long must a simple pendulum be to have a period of 1.5 s? Use g = 9.81 m/s². Find L.

T = 1.5 sg = 9.81 m/s²
L = m
14.Springs & pendulumsHard
t (s)x (cm)t = ?14.4

A body oscillates in simple harmonic motion with period 0.4 s and amplitude 16 cm. What is the shortest time t it needs to move from its maximum displacement of 16 cm to a displacement of 14.4 cm?

T = 0.4 sA = 16 cmx = 14.4 cm
t = s
15.Waves, sound & opticsMedium
75 dB?2 m20 m

A small source sends sound equally in all directions. The level is 75 dB at 2 m from it. Find the level β2 at 20 m, ignoring absorption and reflections.

β1 = 75 dBr1 = 2 mr2 = 20 m
β2 = dB
16.Waves, sound & opticsHard
λ = 589 nmd = 0.1 mmL = 1.5 my = ?

Light of wavelength 589 nm falls on two slits 0.1 mm apart. The screen is 1.5 m away. Find the distance y1 from the central bright fringe to bright fringe number 1.

λ = 589 nmd = 0.1 mmL = 1.5 mm = 1
y1 = mm

3Solutions

1.Kinematics

Answer: s = 9.091 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 = 36/3.6 = 10 m/s

Braking distance

0 = v₀² − 2·a·s → s = v₀²/(2a) = 10²/(2·5.5) = 9.091 m

Answer

s = 9.091 m
2.Kinematics

Answer: y = 16.29 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.

Meeting time

Up is positive, the ground is y = 0.

20 − ½g·t² = 23·t − ½g·t² → t = 20/23 = 0.8696 s

Meeting height

y = 23·0.8696 − ½·9.81·0.8696² = 16.29 m

Answer

y = 16.29 m
3.Newton’s laws

Answer: a = 1.453 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.

Normal force

N = m·g − F·sin θ = 392.4 − 200·sin 25° = 307.9 N

Horizontal forces

m·a = F·cos θ − μ·N = 181.3 − 123.2
a = 58.11/40 = 1.453 m/s²

Answer

a = 1.453 m/s²
4.Newton’s laws

Answer: a = 5.763 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) = (49.05 − 2.943)/8 = 5.763 m/s²

Answer

a = 5.763 m/s²
5.Projectile motion

Answer: θ = 28.19 °

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 = 9.81·110/36² = 0.8326

Angle

2θ = 56.37° → θ = 28.19°

Answer

θ = 28.19°

The other solution is 90° − θ = 61.81°.

6.Projectile motion

Answer: x = 123.4 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 = 22.37 m/s, vy = 31.95 m/s

Time to land on the roof

Larger root: the ball is descending.

27 = 31.95·t − 4.905·t²
t = (31.95 + √(31.95² − 2·9.81·27))/9.81 = 5.515 s

Horizontal distance

x = vx·t = 22.37·5.515 = 123.4 m

Answer

x = 123.4 m
7.Circular motion

Answer: vmax = 20.78 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) = √(0.8·9.81·55) = 20.78 m/s

Answer

vmax = 20.78 m/s (74.79 km/h)
8.Circular motion

Answer: T = 153.3 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 = 1.7·9.81 + 1.7·7.5²/0.7 = 16.68 + 136.6 = 153.3 N

Answer

T = 153.3 N
9.Work & energy

Answer: v = 6.601 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 = √(2·9.81·6·(0.5 − 0.15·0.866)) = 6.601 m/s

Answer

v = 6.601 m/s
10.Work & energy

Answer: v = 7.278 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 left after the rough strip

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

mgh − μmgL = 19.62·(3 − 0.2·1.5) = 52.97 J

Speed at the spring

½mv² = mg(h − μL) → v = √(2g(h − μL)) = √(2·9.81·2.7) = 7.278 m/s

Answer

v = 7.278 m/s
11.Momentum & collisions

Answer: v = 276.9 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) = √(2·9.81·0.11) = 1.469 m/s

Collision

m·v = (m + M)·V → v = (0.008 + 1.5)·1.469/0.008 = 276.9 m/s

Answer

v = 276.9 m/s
12.Momentum & collisions

Answer: J = 3.3 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·(12 + 21) = 3.3 N·s

Answer

J = 3.3 N·s
13.Springs & pendulums

Answer: L = 0.5591 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·(1.5/2π)² = 0.5591 m

Answer

L = 0.5591 m
14.Springs & pendulums

Answer: t = 0.02871 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 = 2π/T = 2π/0.4 = 15.71 rad/s

Solve for the time

0.9 = cos(ω·t) → ω·t = arccos(0.9) = 0.451 rad
t = 0.451/15.71 = 0.02871 s

Answer

t = 0.02871 s
15.Waves, sound & optics

Answer: β2 = 55 dB

Waves: a periodic wave moves one wavelength in one period, so v = fλ with T = 1/f. On a stretched string v = √(T/μ), with T the tension and μ = m/L the mass per metre. Sound in air travels at about 343 m/s at 20 °C, light in vacuum at c = 3.00 × 10⁸ m/s. Loudness is measured on a logarithmic scale: β = 10·log₁₀(I/I₀) dB with I₀ = 10⁻¹² W/m², so 10 times the intensity adds 10 dB. A point source spreads its power P over a sphere: I = P/(4πr²).

Intensity ratio

I₂/I₁ = (2/20)² = 0.01

New level

β₂ = 75 + 10·log₁₀(0.01) = 55 dB

Answer

β2 = 55 dB

Every doubling of the distance lowers the level by about 6 dB.

16.Waves, sound & optics

Answer: y1 = 8.835 mm

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, …

Fringe spacing

Δy = λL/d = 589 × 10⁻⁹·1.5/(0.1 × 10⁻³) = 8.835 mm

Fringe number 1

y1 = 1·8.835 = 8.835 mm

Answer

y1 = 8.835 mm

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