Dynamics: cram pack

Formula sheets, the key method steps for every topic and 20 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.

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

  1. Choose the axis: a fixed pivot, or the centre of mass for rolling bodies.
  2. Find the moment of inertia about that axis from the standard results, using I = IG + m·d² for a shifted axis.
  3. 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.
  4. 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
policea = 5 m/s²car26 m/s

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
AB: 13 m/s25 m

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
10 kg20°F = 100 Nμ = 0.3

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
m1​ = 4 kg5.5 kgno friction

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
v0​ = 16 m/s55°x = ?

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
h = 35 mv0​ = 21 m/s40°v = ?

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
r = 125 mvmax​ = ?

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
r = 1 mv = 9 m/s

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
35°d = 2 mμ = 0.25

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
h = 4.5 mL = 3.5 mμ = 0.15k = 4000 N/m

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
900 kg6 m/s1700 kg

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
11 m/s19 m/s

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
13.5 kgaαM = 10 kgR = 0.15 m

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
400 m/s35 g0.36 mL = 0.9 m3 kgφ

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
N1​ = 18N2​ = 30

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 = 45B = 72C = 15D = 32

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.

P = 1.5 kWnin = 1440 rpmA = 45B = 72C = 15D = 32ηmesh = 98%
Tout = N·m
17.Springs & pendulumsMedium
L = 0.4 m

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
0.7 kgk = 200 N/mA = 10 cm

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
k = 12 kN/mc = 310 N·s/mm = 8 kg

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
k1​ = 80k2​ = 100m = 25 kg

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.

Acceleration of the system

a = (m2·g − μ·m1·g)/(m1 + m2) = (53.96 − 0)/9.5 = 5.679 m/s²

Answer

a = 5.679 m/s²
5.Projectile motion

Answer: x = 24.52 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 = 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.

Block and pulley

block: m·g − T = m·a
pulley: T·R = I·α = ½·M·R²·(a/R) → T = ½·M·a

Acceleration

a = m·g/(m + M/2) = 13.5·9.81/(13.5 + 5) = 7.159 m/s²

Angular acceleration

α = a/R = 7.159/0.15 = 47.72 rad/s²

Answer

α = 47.72 rad/s²
14.Rigid-body rotation

Answer: φ = 99.58 °

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.

Moment of inertia after the impact

I = M·L²/3 + m·d² = 3·0.9²/3 + 0.035·0.36² = 0.8145 kg·m²

Angular momentum about the pivot

The pivot force passes through the pivot, so it has no moment there during the impact.

m·v·d = I·ω → ω = 0.035·400·0.36/0.8145 = 6.188 rad/s

Energy during the swing

½·I·ω² = ½·0.8145·6.188² = 15.59 J
(M·g·L/2 + m·g·d)·(1 − cos φ) = 13.37·(1 − cos φ)
cos φ = 1 − 15.59/13.37 = −0.1665 → φ = 99.58°

Answer

φ = 99.58°
15.Gears & gear trains

Answer: T1 = 74.6 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.

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.

1/keq = 1/80 + 1/100 → keq = 80·100/(80 + 100) = 44.44 kN/m

Answer

keq = 44.44 kN/m

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