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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 driving at 100 km/h brakes with a constant deceleration of 4.5 m/s² until it stops. How long does braking take? Find t.
v₀ = 100 km/ha = −4.5 m/s²v = 0
t = s
2.KinematicsHard
Ball A is dropped from rest from a height of 30 m. At the same instant ball B is thrown straight up from the ground directly below at 27 m/s. Ignore air resistance and use g = 9.81 m/s². At what height y above the ground do they meet?
H = 30 mv0B = 27 m/sg = 9.81 m/s²
y = m
3.Newton’s lawsMedium
An 11 kg block slides down a slope at 45° 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 = 11 kgθ = 45°μ = 0.3g = 9.81 m/s²
a = m/s²
4.Newton’s lawsHard
A 3 kg block on a horizontal table is connected by a light string over a frictionless pulley to a hanging 2 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 = 3 kgm2 = 2 kgμ = 0.25g = 9.81 m/s²
a = m/s²
5.Projectile motionMedium
A ball is launched at 70° above horizontal from level ground. Ignore air resistance. Find the maximum height H the ball reaches.
v0 = 32 m/sθ = 70°g = 9.81 m/s²
H = m
6.Projectile motionHard
A ball is launched at 13 m/s and 35° above the horizontal from the top of a 35 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 = 13 m/sθ = 35°h = 35 mg = 9.81 m/s²
α = °
7.Circular motionMedium
In a fairground rotor, riders stand against the wall of a vertical cylinder of radius 3.5 m. When it spins fast enough the floor drops away and friction holds them up. The coefficient of static friction is 0.4. Use g = 9.81 m/s². Find the smallest rotation rate n in revolutions per minute.
r = 3.5 mμs = 0.4g = 9.81 m/s²
n = rpm
8.Circular motionHard
A 3 kg cart is released from rest at a height of 25.2 m on a frictionless track and runs through a vertical loop of radius 7 m. Use g = 9.81 m/s². Find the normal force Ntop of the track on the cart at the top of the loop.
m = 3 kgh = 25.2 mR = 7 mg = 9.81 m/s²
Ntop = N
9.Work & energyMedium
A block slides from rest down a slope at 35° to the horizontal. The coefficient of kinetic friction is 0.35. Find its speed v after it has slid 14 m along the slope.
θ = 35°μ = 0.35d = 14 mg = 9.81 m/s²
v = m/s
10.Work & energyHard
A 5 kg block is released from rest at height 5 m on a smooth ramp. At the bottom it crosses a rough horizontal strip 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 = 5 kgh = 5 mL = 5 mμ = 0.15k = 2000 N/mg = 9.81 m/s²
x = cm
11.Momentum & collisionsMedium
An 8 g bullet is fired horizontally into a 2.5 kg wooden block hanging on light strings, and stays inside it. The block swings up until it is 19 cm higher than at the start. Use g = 9.81 m/s². Find the speed v of the bullet before impact.
m = 8 gM = 2.5 kgh = 19 cmg = 9.81 m/s²
v = m/s
12.Momentum & collisionsHard
A 0.2 kg ball hits a wall at 25 m/s and bounces straight back at 20 m/s. The contact lasts 40 ms. Find the average force Favg of the wall on the ball.
m = 0.2 kgvin = 25 m/svout = 20 m/sΔt = 40 ms
Favg = N
13.Rigid-body rotationMedium
An 8.5 kg block hangs from a light cord wrapped around a pulley, a uniform solid disc of mass 18.5 kg and radius 0.15 m that turns on a frictionless horizontal axle. The block is released from rest. Use g = 9.81 m/s². Find the angular acceleration α of the pulley.
m = 8.5 kgM = 18.5 kgR = 0.15 mg = 9.81 m/s²
α = rad/s²
14.Rigid-body rotationHard
A uniform slender rod of mass 4.5 kg and length 0.8 m hangs at rest from a frictionless pivot at its top end. A 25 g bullet moving horizontally at 320 m/s hits the rod 0.72 m below the pivot and stays embedded. Find the angular velocity ω of the rod just after the impact.
M = 4.5 kgL = 0.8 mm = 25 gv = 320 m/sd = 0.72 m
ω = rad/s
15.Gears & gear trainsMedium
A 7.5 kW motor running at 1500 rpm drives a pinion with 20 teeth, which meshes with a gear with 30 teeth. The gear pair has an efficiency of 95%. Find the output torque T2 on the gear shaft.
P = 7.5 kWn1 = 1500 rpmN1 = 20N2 = 30η = 95%
T2 = N·m
16.Gears & gear trainsHard
A 7.5 kW motor at 1440 rpm drives gear A (15 teeth), which meshes with gear B (18 teeth). Gear C (40 teeth) on the same shaft as B drives gear D (60 teeth) on the output shaft. Each gear mesh has an efficiency of 98%. Find the output torque Tout.
How long must a simple pendulum be to have a period of 1.6 s? Use g = 9.81 m/s². Find L.
T = 1.6 sg = 9.81 m/s²
L = m
18.Springs & pendulumsHard
A body oscillates in simple harmonic motion with period 3.5 s and amplitude 9 cm. What is the shortest time t it needs to move from its maximum displacement of 9 cm to a displacement of 4.5 cm?
T = 3.5 sA = 9 cmx = 4.5 cm
t = s
19.Mechanical vibrationsMedium
In a free-vibration test of a damped mass–spring system, a displacement peak of 20 mm is followed 4 cycles later by a peak of 5.7 mm. Find the damping ratio ζ.
x0 = 20 mmx4 = 5.7 mmn = 4
ζ =
20.Mechanical vibrationsHard
A 5 kg mass hangs from two springs connected end to end (in series): the upper spring has k₁ = 60 kN/m and the lower one k₂ = 5 kN/m. Find the equivalent stiffness keq of the spring system in kN/m.
m = 5 kgk1 = 60 kN/mk2 = 5 kN/m
keq = kN/m
3Solutions
1.Kinematics
Answer: t = 6.173 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 = 100/3.6 = 27.78 m/s
Braking time
0 = v₀ − a·t → t = v₀/a = 27.78/4.5 = 6.173 s
Answer
t = 6.173 s
2.Kinematics
Answer: y = 23.94 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.
30 − ½g·t² = 27·t − ½g·t² → t = 30/27 = 1.111 s
Meeting height
y = 27·1.111 − ½·9.81·1.111² = 23.94 m
Answer
y = 23.94 m
3.Newton’s laws
Answer: a = 4.856 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.
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.
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 = 32·cos 70° = 10.94 m/s
vy = v0·sin θ = 32·sin 70° = 30.07 m/s
Highest point
At the top the vertical velocity is zero: vy² = 2gH.
H = vy²/(2g) = 30.07²/(2·9.81) = 46.09 m
Answer
H = 46.09 m
6.Projectile motion
Answer: α = 68.65 °
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 = 13·cos 35° = 10.65 m/s
vy0 = 13·sin 35° = 7.456 m/s
Vertical speed at impact
Energy or v² = v₀² + 2as in the vertical direction.
vy = √(7.456² + 2·9.81·35) = 27.25 m/s
Impact angle
tan α = vy/vx = 27.25/10.65 → α = 68.65°
Answer
α = 68.65°
7.Circular motion
Answer: n = 25.28 rpm
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 on a rider
N = m·ω²·r
μ·N = m·g → μ·ω²·r = g
Angular speed
ω = √(g/(μ·r)) = √(9.81/(0.4·3.5)) = 2.647 rad/s
Rotation rate
n = ω·60/(2π) = 25.28 rpm
Answer
n = 25.28 rpm
8.Circular motion
Answer: Ntop = 64.75 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 from energy conservation
v² = 2·9.81·(25.2 − 2·7) = 219.7 m²/s²
Forces
Towards the centre is positive.
N = m·v²/R − m·g = 3·219.7/7 − 29.43 = 64.75 N
Answer
Ntop = 64.75 N
9.Work & energy
Answer: v = 8.877 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 = √(2·9.81·14·(0.5736 − 0.35·0.8192)) = 8.877 m/s
Answer
v = 8.877 m/s
10.Work & energy
Answer: x = 45.66 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 = 49.05·(5 − 0.15·5) = 208.5 J
Maximum compression
½kx² = 208.5 → x = √(2·208.5/2000) = 0.4566 m = 45.66 cm
Answer
x = 45.66 cm
11.Momentum & collisions
Answer: v = 605.3 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) = √(2·9.81·0.19) = 1.931 m/s
Collision
m·v = (m + M)·V → v = (0.008 + 2.5)·1.931/0.008 = 605.3 m/s
Answer
v = 605.3 m/s
12.Momentum & collisions
Answer: Favg = 225 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 = 0.2·(20 + 25) = 9 N·s
Average force
Favg = J/Δt = 9/0.04 = 225 N
Answer
Favg = 225 N
13.Rigid-body rotation
Answer: α = 31.32 rad/s²
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.
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.
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.
Motor torque
ω₁ = 2π·1500/60 = 157.1 rad/s
T1 = P/ω₁ = 7500/157.1 = 47.75 N·m
Output torque
T2 = 47.75·30/20·0.95 = 68.04 N·m
Answer
T2 = 68.04 N·m
16.Gears & gear trains
Answer: Tout = 85.98 N·m
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.
Output speed
nout = 1440·(15/18)·(40/60) = 800 rpm
ωout = 2π·800/60 = 83.78 rad/s
Output power and torque
Pout = 7500·0.98² = 7203 W
Tout = Pout/ωout = 7203/83.78 = 85.98 N·m
Answer
Tout = 85.98 N·m
17.Springs & pendulums
Answer: L = 0.6361 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·(1.6/2π)² = 0.6361 m
Answer
L = 0.6361 m
18.Springs & pendulums
Answer: t = 0.5833 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/3.5 = 1.795 rad/s
Solve for the time
0.5 = cos(ω·t) → ω·t = arccos(0.5) = 1.047 rad
t = 1.047/1.795 = 0.5833 s
Answer
t = 0.5833 s
19.Mechanical vibrations
Answer: ζ = 0.04988
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.
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.