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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
List what you know: v₀, v, a, t and s, with units.
Pick the equation that contains your three knowns and the unknown.
Choose one positive direction and give opposing quantities a minus sign.
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
Draw a free-body diagram with every force on the body.
Choose a positive direction along the motion.
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).
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
Split the launch velocity into components: vx = v₀·cos θ and vy = v₀·sin θ.
The horizontal motion has constant speed; the vertical motion has acceleration −g.
Find the time of flight from the vertical motion.
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
Choose a positive direction and give each velocity its sign.
Write the total momentum before: Σm·v.
For a perfectly inelastic collision the bodies move together after; for an elastic one kinetic energy is also conserved.
Set momentum before equal to momentum after and solve.
Rigid-body rotation
Moments of inertia about G
rod mL²/12, disc ½mR², ring mR², solid sphere (2/5)mR², hollow sphere (2/3)mR²
Parallel-axis theorem
I = IG + m·d²
Radius of gyration
I = m·k²
Rod about its end
I = mL²/3
Equation of motion
ΣM = I·α
Speed in rad/s
ω = 2π·n/60
Kinetic energy
E = ½·I·ω²
Work and power
W = T·θ, P = T·ω
Rolling without slipping
v = ω·r, E = ½mv²(1 + I/(mr²)), a = g·sin θ/(1 + I/(mr²))
Angular momentum
L = I·ω, I1ω1 = I2ω2
Impact about a pivot
m·v·d = I·ω
Method
Choose the axis: a fixed pivot, or the centre of mass for rolling bodies.
Find the moment of inertia about that axis from the standard results, using I = IG + m·d² for a shifted axis.
Pick the method: ΣM = I·α for accelerations and forces, energy (½·I·ω² + ½·m·v² + m·g·h) for speeds, angular momentum for impacts and sudden changes.
Link linear and angular motion with v = ω·r and a = α·r, and convert rpm to rad/s.
Gears & gear trains
Meshing gears
n1·N1 = n2·N2
Torque
T2 = T1·(N2/N1)·η
Power
P = T·ω, ω = 2π·n/60
Compound train
total ratio = product of the stage ratios
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
Mechanical vibrations
Natural frequency
ωn = √(k/m), fn = ωn/(2π)
From static deflection
ωn = √(g/δst)
Critical damping
cc = 2√(km) = 2mωn
Damping ratio
ζ = c/cc
Damped frequency
ωd = ωn√(1 − ζ²)
Logarithmic decrement
δ = (1/n)·ln(x0/xn), ζ = δ/√(4π² + δ²)
Springs in parallel
k = k1 + k2
Springs in series
1/k = 1/k1 + 1/k2
2Practice problems
1.KinematicsMedium
A car speeding at a constant 18 m/s passes a police car standing still. At that moment the police car starts and accelerates uniformly at 3.5 m/s². How far from its starting point does the police car catch up? Find d.
vcar = 18 m/sapolice = 3.5 m/s²v0,police = 0
d = m
2.KinematicsHard
A tram starts from rest and accelerates at 2 m/s² for 10 s, then runs at constant speed for 14 s, and finally brakes at 4 m/s² until it stops. Find the total travel time t.
a1 = 2 m/s²t1 = 10 st2 = 14 sa3 = −4 m/s²
t = s
3.Newton’s lawsMedium
A 40 kg sled is pulled across level snow by a rope at 30° above the horizontal with a force of 100 N. The coefficient of kinetic friction is 0.2. Use g = 9.81 m/s². Find the acceleration a of the sled.
m = 40 kgF = 100 Nθ = 30°μ = 0.2g = 9.81 m/s²
a = m/s²
4.Newton’s lawsHard
A block is given a push so that it starts sliding up a ramp at 35° with a speed of 9 m/s. The coefficient of kinetic friction is 0.25. Use g = 9.81 m/s². How far d along the ramp does it slide before it stops?
v₀ = 9 m/sθ = 35°μ = 0.25g = 9.81 m/s²
d = m
5.Projectile motionMedium
A ball is launched from level ground at 55° above the horizontal and lands 90 m away. Ignore air resistance and use g = 9.81 m/s². Find the launch speed v0.
θ = 55°R = 90 mg = 9.81 m/s²
v0 = m/s
6.Projectile motionHard
A ball is launched at 11 m/s and 55° above the horizontal from the top of a 25 m cliff. Ignore air resistance and use g = 9.81 m/s². At what angle α below the horizontal does it hit the ground?
v₀ = 11 m/sθ = 55°h = 25 mg = 9.81 m/s²
α = °
7.Circular motionMedium
A small ball on a string of length 1.2 m moves in a horizontal circle so that the string makes a constant angle of 45° with the vertical (a conical pendulum). Use g = 9.81 m/s². Find the speed v of the ball.
L = 1.2 mθ = 45°g = 9.81 m/s²
v = m/s
8.Circular motionHard
A 0.4 kg ball on a light string 0.6 m long is swung in a vertical circle. At the lowest point its speed is 8 m/s. Ignore air resistance and use g = 9.81 m/s². Find the tension Ttop in the string at the highest point.
m = 0.4 kgr = 0.6 mvbottom = 8 m/sg = 9.81 m/s²
Ttop = N
9.Work & energyMedium
A 5 kg block slides 9 m down a slope at 45° to the horizontal, with a coefficient of kinetic friction of 0.25. Find the work Wf done against friction.
m = 5 kgθ = 45°μ = 0.25d = 9 mg = 9.81 m/s²
Wf = J
10.Work & energyHard
A spring of stiffness 3000 N/m at the bottom of a 40° slope is compressed by 12 cm against a 2 kg block and released. The coefficient of kinetic friction between block and slope is 0.2. 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.)
An 11 kg projectile moving horizontally at 24 m/s explodes into two fragments that move along the same line. The 10 kg fragment continues forwards at 47 m/s. Find the velocity v′2 of the 1 kg fragment (positive in the original direction).
M = 11 kgu = 24 m/sm1 = 10 kgv′1 = 47 m/sm2 = 1 kg
v′2 = m/s
12.Momentum & collisionsHard
A 0.15 kg ball hits a wall at 27 m/s and bounces straight back at 17 m/s. The contact lasts 10 ms. Find the magnitude of the impulse J the wall gives the ball.
m = 0.15 kgvin = 27 m/svout = 17 m/sΔt = 10 ms
J = N·s
13.Rigid-body rotationMedium
A flywheel with a moment of inertia of 35.5 kg·m² spins at 2800 rpm. A brake applies a constant friction torque of 190 N·m. How many revolutions N does the flywheel make before it stops?
I = 35.5 kg·m²n = 2800 rpmTb = 190 N·m
N = rev
14.Rigid-body rotationHard
A thin hoop starts from rest and rolls without slipping down a slope inclined at 25° to the horizontal. Use g = 9.81 m/s². Its radius is 0.25 m. Find its angular velocity ω after it has rolled 1.5 m along the slope.
θ = 25°s = 1.5 mI = m·r²g = 9.81 m/s²r = 0.25 m
ω = rad/s
15.Gears & gear trainsMedium
A 2.2 kW motor running at 1450 rpm drives a pinion with 24 teeth and a module of 2 mm. Find the tangential force Ft on the pinion teeth.
P = 2.2 kWn = 1450 rpmN1 = 24m = 2 mm
Ft = N
16.Gears & gear trainsHard
In a compound gear train, gear A (18 teeth) on the input shaft turning at 1500 rpm drives gear B (80 teeth). Gear C (18 teeth) is fixed to the same shaft as B and drives gear D (25 teeth) on the output shaft. Find the output speed nout.
nin = 1500 rpmA = 18B = 80C = 18D = 25
nout = rpm
17.Springs & pendulumsMedium
A 0.3 kg mass on a spring with k = 190 N/m is pulled 3 cm in the positive direction and released from rest at t = 0. Find its displacement x from equilibrium at t = 1 s (with sign).
m = 0.3 kgk = 190 N/mA = 3 cmt = 1 s
x = cm
18.Springs & pendulumsHard
A 3.6 kg mass on a spring with k = 310 N/m is pulled 9 cm from equilibrium and released. Find the total energy E of the oscillation.
m = 3.6 kgk = 310 N/mA = 9 cm
E = J
19.Mechanical vibrationsMedium
An 80 kg mass is supported by a spring with a stiffness of 200 kN/m and a viscous damper with a damping coefficient of 4000 N·s/m. Find the damping ratio ζ.
m = 80 kgk = 200 kN/mc = 4000 N·s/m
ζ =
20.Mechanical vibrationsHard
A 10 kg mass hangs from two springs connected end to end (in series): the upper spring has k₁ = 30 kN/m and the lower one k₂ = 50 kN/m. Find the equivalent stiffness keq of the spring system in kN/m.
m = 10 kgk1 = 30 kN/mk2 = 50 kN/m
keq = kN/m
3Solutions
1.Kinematics
Answer: d = 185.1 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.
Equal distances
v·t = ½·a·t² → t = 2v/a = 2·18/3.5 = 10.29 s
Distance
d = v·t = 18·10.29 = 185.1 m
Answer
d = 185.1 m
At that moment the police car moves at 2v = 36 m/s.
2.Kinematics
Answer: t = 29 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 = 2·10 = 20 m/s
Braking time
t3 = v/a3 = 20/4 = 5 s
Total time
t = 10 + 14 + 5 = 29 s
Answer
t = 29 s
3.Newton’s laws
Answer: a = 0.4531 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 − 100·sin 30° = 342.4 N
Horizontal forces
m·a = F·cos θ − μ·N = 86.6 − 68.48
a = 18.12/40 = 0.4531 m/s²
Answer
a = 0.4531 m/s²
4.Newton’s laws
Answer: d = 5.304 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° + 0.25·cos 35°) = 7.636 m/s²
Distance
d = v₀²/(2a) = 9²/(2·7.636) = 5.304 m
Answer
d = 5.304 m
5.Projectile motion
Answer: v0 = 30.65 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) = √(9.81·90/sin 110°) = 30.65 m/s
Answer
v0 = 30.65 m/s
6.Projectile motion
Answer: α = 75.22 °
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·cos 55° = 6.309 m/s
vy0 = 11·sin 55° = 9.011 m/s
Vertical speed at impact
Energy or v² = v₀² + 2as in the vertical direction.
vy = √(9.011² + 2·9.81·25) = 23.91 m/s
Impact angle
tan α = vy/vx = 23.91/6.309 → α = 75.22°
Answer
α = 75.22°
7.Circular motion
Answer: v = 2.885 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.
Radius of the circle
r = L·sin θ = 1.2·sin 45° = 0.8485 m
Speed
Tension and gravity together give the inward force: tan θ = v²/(r·g).
v = √(r·g·tan θ) = √(0.8485·9.81·tan 45°) = 2.885 m/s
Answer
v = 2.885 m/s
8.Circular motion
Answer: Ttop = 23.05 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 = 8² − 4·9.81·0.6 = 40.46 m²/s²
Forces at the top
Tension and gravity both point down, towards the centre.
T + m·g = m·vtop²/r
T = 0.4·40.46/0.6 − 0.4·9.81 = 23.05 N
Answer
Ttop = 23.05 N
9.Work & energy
Answer: Wf = 78.04 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 = 49.05·0.7071 = 34.68 N
F = μN = 0.25·34.68 = 8.671 N
Work against friction
Wf = F·d = 8.671·9 = 78.04 J
Answer
Wf = 78.04 J
10.Work & energy
Answer: d = 1.383 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 = 12 cm = 0.12 m
½kx² = ½·3000·0.12² = 21.6 J
Energy balance along the slope
m·g = 2·9.81 = 19.62 N
½kx² = mg·d·(sin θ + μ·cos θ)
d = 21.6/(19.62·(0.6428 + 0.2·0.766)) = 1.383 m
Answer
d = 1.383 m
11.Momentum & collisions
Answer: v′2 = −206 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.
Momentum before
p = M·u = 11·24 = 264 kg·m/s
Momentum after
264 = 10·47 + 1·v′2
v′2 = (264 − 470)/1 = −206 m/s
Answer
v′2 = −206 m/s
The minus sign means the second fragment flies backwards.
12.Momentum & collisions
Answer: J = 6.6 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 = 0.15·(17 + 27) = 6.6 N·s
Answer
J = 6.6 N·s
13.Rigid-body rotation
Answer: N = 1278 rev
Rotation about a fixed axis: the sum of the moments about the axis equals I·α (ΣM = I·α), just as ΣF = m·a for translation. In energy form, a torque T turning through an angle θ (in radians) does work T·θ, which changes the kinetic energy ½·I·ω²; gravity adds or removes m·g·Δh of the centre of mass. Power is P = T·ω.
Angular velocity
ω = 2π·2800/60 = 293.2 rad/s
Work of the brake equals the kinetic energy
½·I·ω² = ½·35.5·293.2² = 1.526 × 10⁶ J
θ = 1.526 × 10⁶/190 = 8032 rad
Revolutions
N = θ/2π = 1278 rev
Answer
N = 1278 rev
14.Rigid-body rotation
Answer: ω = 9.975 rad/s
Rolling and angular momentum: a body rolling without slipping has v = ω·r, so its kinetic energy is ½·m·v² + ½·I·ω² = ½·m·v²·(1 + I/(m·r²)). Down a slope that gives a = g·sin θ/(1 + I/(m·r²)). When no external moment acts about an axis, the angular momentum about that axis stays constant, I₁·ω₁ = I₂·ω₂, even if kinetic energy is lost.
Height dropped
h = s·sin θ = 1.5·sin 25° = 0.6339 m
Energy balance with rolling
Rolling without slipping: ω = v/r, and friction does no work at the contact point.
m·g·h = ½·m·v²·(1 + 1)
v = √(2·9.81·0.6339/2) = 2.494 m/s
ω = v/r = 2.494/0.25 = 9.975 rad/s
Answer
ω = 9.975 rad/s
15.Gears & gear trains
Answer: Ft = 603.7 N
Gear geometry: the module m sets the tooth size. A gear with N teeth has a pitch diameter d = m·N, two meshing gears have the same module, and their centre distance is a = (d₁ + d₂)/2 = m·(N₁ + N₂)/2. The pitch-line speed is v = π·d·n/60, and the tangential tooth force follows from the torque: Ft = 2T/d.
Torque on the pinion
ω = 2π·1450/60 = 151.8 rad/s
T = P/ω = 2200/151.8 = 14.49 N·m
Pitch diameter
d = m·N = 2·24 = 48 mm
Tangential force
Ft = 2T/d = 2·14.49/0.048 = 603.7 N
Answer
Ft = 603.7 N
16.Gears & gear trains
Answer: nout = 243 rpm
Gear trains: meshing gears have the same speed at the teeth, so n₁·N₁ = n₂·N₂: the gear with fewer teeth turns faster. Gears on one shaft turn at the same speed. Power is passed on (minus losses), so torque goes up when speed goes down: T₂ = T₁·(N₂/N₁)·η, and P = T·ω with ω = 2π·n/60.
First stage
nB = 1500·18/80 = 337.5 rpm = nC
Second stage
nout = 337.5·18/25 = 243 rpm
Answer
nout = 243 rpm
total ratio = 6.173 : 1
17.Springs & pendulums
Answer: x = 2.998 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.
Angular frequency
ω = √(190/0.3) = 25.17 rad/s
ω·t = 25.17·1 = 25.17 rad
Displacement
x = A·cos(ω·t) = 3·cos(25.17) = 2.998 cm
Answer
x = 2.998 cm
18.Springs & pendulums
Answer: E = 1.255 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.
Angular frequency
ω = √(310/3.6) = 9.28 rad/s
Energy
E = ½·k·A² = ½·310·0.09² = 1.255 J
Answer
E = 1.255 J
19.Mechanical vibrations
Answer: ζ = 0.5
Free vibration of a mass–spring system: the undamped natural frequency is ωn = √(k/m) in rad/s, and fn = ωn/(2π) in Hz. A viscous damper c gives the damping ratio ζ = c/cc, with critical damping cc = 2·√(k·m) = 2·m·ωn. An underdamped system (ζ < 1) oscillates at ωd = ωn·√(1 − ζ²). Springs in parallel add, k = k₁ + k₂; springs in series add as reciprocals, 1/k = 1/k₁ + 1/k₂.
Critical damping
cc = 2·√(k·m) = 2·√(200000·80) = 8000 N·s/m
Damping ratio
ζ = c/cc = 4000/8000 = 0.5
Answer
ζ = 0.5
ζ < 1, so the system is underdamped and oscillates as it decays.
20.Mechanical vibrations
Answer: keq = 18.75 kN/m
Free vibration of a mass–spring system: the undamped natural frequency is ωn = √(k/m) in rad/s, and fn = ωn/(2π) in Hz. A viscous damper c gives the damping ratio ζ = c/cc, with critical damping cc = 2·√(k·m) = 2·m·ωn. An underdamped system (ζ < 1) oscillates at ωd = ωn·√(1 − ζ²). Springs in parallel add, k = k₁ + k₂; springs in series add as reciprocals, 1/k = 1/k₁ + 1/k₂.
Equivalent stiffness
Springs in series share the same force and add their deflections, so they combine as reciprocals: 1/k = 1/k1 + 1/k2.