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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 26 m/s passes a police car standing still. At that moment the police car starts and accelerates uniformly at 5 m/s². How long does it take the police car to catch up? Find t.
vcar = 26 m/sapolice = 5 m/s²v0,police = 0
t = s
2.KinematicsHard
Ball A is dropped from rest from a height of 25 m. At the same instant ball B is thrown straight up from the ground directly below at 13 m/s. Ignore air resistance and use g = 9.81 m/s². At what height y above the ground do they meet?
H = 25 mv0B = 13 m/sg = 9.81 m/s²
y = m
3.Newton’s lawsMedium
A 10 kg sled is pulled across level snow by a rope at 20° above the horizontal with a force of 100 N. The coefficient of kinetic friction is 0.3. Use g = 9.81 m/s². Find the acceleration a of the sled.
m = 10 kgF = 100 Nθ = 20°μ = 0.3g = 9.81 m/s²
a = m/s²
4.Newton’s lawsHard
A 4 kg block on a horizontal table is connected by a light string over a frictionless pulley to a hanging 5.5 kg mass. The table is frictionless. Use g = 9.81 m/s². Find the acceleration a of the system.
m1 = 4 kgm2 = 5.5 kgμ = 0g = 9.81 m/s²
a = m/s²
5.Projectile motionMedium
A ball is launched at 55° above horizontal from level ground. Ignore air resistance. Find the horizontal distance x travelled before the ball hits the ground.
v0 = 16 m/sθ = 55°g = 9.81 m/s²
x = m
6.Projectile motionHard
A ball is launched at 21 m/s and 40° above the horizontal from the top of a 35 m cliff. Ignore air resistance and use g = 9.81 m/s². Find the speed v with which it hits the ground.
v₀ = 21 m/sθ = 40°h = 35 mg = 9.81 m/s²
v = m/s
7.Circular motionMedium
A car takes a flat curve of radius 125 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 = 125 mμs = 0.8g = 9.81 m/s²
vmax = m/s
8.Circular motionHard
A 1.6 kg ball on a string 1 m long is swung in a vertical circle. At the lowest point it moves at 9 m/s. Use g = 9.81 m/s². Find the tension T in the string at the lowest point.
m = 1.6 kgr = 1 mv = 9 m/sg = 9.81 m/s²
T = N
9.Work & energyMedium
A block slides from rest down a slope at 35° to the horizontal. The coefficient of kinetic friction is 0.25. Find its speed v after it has slid 2 m along the slope.
θ = 35°μ = 0.25d = 2 mg = 9.81 m/s²
v = m/s
10.Work & energyHard
A 4 kg block is released from rest at height 4.5 m on a smooth ramp. At the bottom it crosses a rough horizontal strip 3.5 m long (μ = 0.15) and then runs onto a spring (k = 4000 N/m) on a smooth surface. Find the maximum compression x of the spring.
m = 4 kgh = 4.5 mL = 3.5 mμ = 0.15k = 4000 N/mg = 9.81 m/s²
x = cm
11.Momentum & collisionsMedium
A 900 kg car moving at 6 m/s runs into a stationary 1700 kg car and the two lock together. What percentage ΔK/K of the original kinetic energy is lost?
m1 = 900 kgv1 = 6 m/sm2 = 1700 kgv2 = 0
ΔK/K = %
12.Momentum & collisionsHard
A 0.15 kg ball hits a wall at 11 m/s and bounces straight back at 19 m/s. The contact lasts 50 ms. Find the average force Favg of the wall on the ball.
m = 0.15 kgvin = 11 m/svout = 19 m/sΔt = 50 ms
Favg = N
13.Rigid-body rotationMedium
A 13.5 kg block hangs from a light cord wrapped around a pulley, a uniform solid disc of mass 10 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 = 13.5 kgM = 10 kgR = 0.15 mg = 9.81 m/s²
α = rad/s²
14.Rigid-body rotationHard
A uniform slender rod of mass 3 kg and length 0.9 m hangs at rest from a frictionless pivot at its top end. A 35 g bullet moving horizontally at 400 m/s hits the rod 0.36 m below the pivot and stays embedded. Use g = 9.81 m/s². Find the largest angle φ from the vertical through which the rod swings.
M = 3 kgL = 0.9 mm = 35 gv = 400 m/sd = 0.36 mg = 9.81 m/s²
φ = °
15.Gears & gear trainsMedium
A 7.5 kW motor running at 960 rpm drives a pinion with 18 teeth, which meshes with a gear with 30 teeth. The gear pair has an efficiency of 97%. Find the torque T1 on the motor shaft.
P = 7.5 kWn1 = 960 rpmN1 = 18N2 = 30η = 97%
T1 = N·m
16.Gears & gear trainsHard
A 1.5 kW motor at 1440 rpm drives gear A (45 teeth), which meshes with gear B (72 teeth). Gear C (15 teeth) on the same shaft as B drives gear D (32 teeth) on the output shaft. Each gear mesh has an efficiency of 98%. Find the output torque Tout.
A simple pendulum has a length of 0.4 m. Use g = 9.81 m/s². Find its period T for small swings.
L = 0.4 mg = 9.81 m/s²
T = s
18.Springs & pendulumsHard
A 0.7 kg mass on a spring with k = 200 N/m is pulled 10 cm from equilibrium and released. Find the total energy E of the oscillation.
m = 0.7 kgk = 200 N/mA = 10 cm
E = J
19.Mechanical vibrationsMedium
An 8 kg mass is supported by a spring with a stiffness of 12 kN/m and a viscous damper with a damping coefficient of 310 N·s/m. Find the damping ratio ζ.
m = 8 kgk = 12 kN/mc = 310 N·s/m
ζ =
20.Mechanical vibrationsHard
A 25 kg mass hangs from two springs connected end to end (in series): the upper spring has k₁ = 80 kN/m and the lower one k₂ = 100 kN/m. Find the equivalent stiffness keq of the spring system in kN/m.
m = 25 kgk1 = 80 kN/mk2 = 100 kN/m
keq = kN/m
3Solutions
1.Kinematics
Answer: t = 10.4 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.
Equal distances
v·t = ½·a·t² → t = 2v/a = 2·26/5 = 10.4 s
Answer
t = 10.4 s
At that moment the police car moves at 2v = 52 m/s.
2.Kinematics
Answer: y = 6.86 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.
25 − ½g·t² = 13·t − ½g·t² → t = 25/13 = 1.923 s
Meeting height
y = 13·1.923 − ½·9.81·1.923² = 6.86 m
Answer
y = 6.86 m
3.Newton’s laws
Answer: a = 7.48 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 = 98.1 − 100·sin 20° = 63.9 N
Horizontal forces
m·a = F·cos θ − μ·N = 93.97 − 19.17
a = 74.8/10 = 7.48 m/s²
Answer
a = 7.48 m/s²
4.Newton’s laws
Answer: a = 5.679 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.
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 = 16·cos 55° = 9.177 m/s
vy = v0·sin θ = 16·sin 55° = 13.11 m/s
Time in the air
Starting and landing at the same height: t = 2vy/g.
t = 2·13.11/9.81 = 2.672 s
Horizontal distance
x = vx·t = 9.177·2.672 = 24.52 m
Answer
x = 24.52 m
6.Projectile motion
Answer: v = 33.58 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.
Split the launch velocity
vx = 21·cos 40° = 16.09 m/s
vy0 = 21·sin 40° = 13.5 m/s
Vertical speed at impact
Energy or v² = v₀² + 2as in the vertical direction.
vy = √(13.5² + 2·9.81·35) = 29.48 m/s
Impact speed
v = √(16.09² + 29.48²) = 33.58 m/s
Answer
v = 33.58 m/s
Check with energy: v² = v₀² + 2gh.
7.Circular motion
Answer: vmax = 31.32 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) = √(0.8·9.81·125) = 31.32 m/s
Answer
vmax = 31.32 m/s (112.8 km/h)
8.Circular motion
Answer: T = 145.3 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 = 1.6·9.81 + 1.6·9²/1 = 15.7 + 129.6 = 145.3 N
Answer
T = 145.3 N
9.Work & energy
Answer: v = 3.804 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 = √(2·9.81·2·(0.5736 − 0.25·0.8192)) = 3.804 m/s
Answer
v = 3.804 m/s
10.Work & energy
Answer: x = 27.93 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 = 39.24·(4.5 − 0.15·3.5) = 156 J
Maximum compression
½kx² = 156 → x = √(2·156/4000) = 0.2793 m = 27.93 cm
Answer
x = 27.93 cm
11.Momentum & collisions
Answer: ΔK/K = 65.38 %
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) = 900·6/2600 = 2.077 m/s
Kinetic energy before and after
Kbefore = ½·900·6² = 16200 J
Kafter = ½·2600·2.077² = 5608 J
Fraction lost
ΔK/K = 10592/16200 = 65.38 %
Answer
ΔK/K = 65.38 %
The lost energy goes into deformation, heat and sound.
12.Momentum & collisions
Answer: Favg = 90 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 = 0.15·(19 + 11) = 4.5 N·s
Average force
Favg = J/Δt = 4.5/0.05 = 90 N
Answer
Favg = 90 N
13.Rigid-body rotation
Answer: α = 47.72 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·960/60 = 100.5 rad/s
T1 = P/ω₁ = 7500/100.5 = 74.6 N·m
Answer
T1 = 74.6 N·m
16.Gears & gear trains
Answer: Tout = 32.61 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·(45/72)·(15/32) = 421.9 rpm
ωout = 2π·421.9/60 = 44.18 rad/s
Output power and torque
Pout = 1500·0.98² = 1441 W
Tout = Pout/ωout = 1441/44.18 = 32.61 N·m
Answer
Tout = 32.61 N·m
17.Springs & pendulums
Answer: T = 1.269 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.
Pendulum period
T = 2π·√(0.4/9.81) = 1.269 s
Answer
T = 1.269 s
18.Springs & pendulums
Answer: E = 1 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 = √(200/0.7) = 16.9 rad/s
Energy
E = ½·k·A² = ½·200·0.1² = 1 J
Answer
E = 1 J
19.Mechanical vibrations
Answer: ζ = 0.5003
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·√(12000·8) = 619.7 N·s/m
Damping ratio
ζ = c/cc = 310/619.7 = 0.5003
Answer
ζ = 0.5003
ζ < 1, so the system is underdamped and oscillates as it decays.
20.Mechanical vibrations
Answer: keq = 44.44 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.