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2025/2026

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SCIENCE OLYMPIAD — MACHINES
Complete Binder Cheat Sheet
Division B & C | 2025–2026 | All Formulas · Concepts · Worked Examples
QUICK FORMULA FLASH
W = F·d | MA = F_out/F_in | IMA = d_in/d_out
η = (AMA/IMA)×100% | τ = F·d_⊥ | ΣF = ma
KE = ½mv² | PE = mgh | p = mv
Page 1: Core Physics & Kinematics Page 2: Simple Machines Overview
Page 3: Levers & Torque In-Depth Page 4: Pulleys & Wheel/Axle
Page 5: Compound Machines, Gears & Efficiency Page 6: Energy, Momentum & Lever Device Tips
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SCIENCE OLYMPIAD — MACHINES

Complete Binder Cheat Sheet

Division B & C | 2025–2026 | All Formulas · Concepts · Worked Examples

⚡ QUICK FORMULA FLASH

W = F·d | MA = F_out/F_in | IMA = d_in/d_out

η = (AMA/IMA)×100% | τ = F·d_⊥ | ΣF = ma

KE = ½mv² | PE = mgh | p = mv

Page 1: Core Physics & Kinematics Page 2: Simple Machines Overview Page 3: Levers & Torque In-Depth Page 4: Pulleys & Wheel/Axle Page 5: Compound Machines, Gears & Efficiency Page 6: Energy, Momentum & Lever Device Tips

PAGE 1 — CORE PHYSICS: FORCES, KINEMATICS & NEWTON'S LAWS Units & Measurement Quantity SI Unit Symbol / Notes

Force Newton N = kg·m/s²

Mass Kilogram kg

Distance / Length Meter m

Work / Energy Joule J = N·m = kg·m²/s²

Power Watt W = J/s

Torque Newton-meter N·m

Velocity / Speed Meters/second m/s

Acceleration Meters/second² m/s²

Momentum kg·m/s p = mv

Frequency Hertz Hz = 1/s

Kinematics — 1D Motion Key quantities: position (x), displacement (Δx), velocity (v), acceleration (a), time (t)

Velocity (avg) v = Δx / Δt^ Δx = final − initial position

Acceleration (avg) a = Δv / Δt^ Units: m/s² — change in velocity over time

Big Four #1 v = v^ ₀^ + a·t Final velocity — no displacement needed

Big Four #2 Δx = v^ ₀ t + ½at²^ Displacement — used when no final v

Big Four #3 v² = v^ ₀ ² + 2aΔx^ No time needed — great for ramps/slides

Big Four #4 Δx = ½(v^ ₀ +v)t^ Avg velocity × time

Free Fall g = 9.8 m/s²^ (≈10)^ Downward acceleration due to gravity

Tip: On inclined planes the acceleration down the slope = g·sin(θ). Normal force = mg·cos(θ). Newton's Three Laws of Motion Law Statement Formula / Key Point

PAGE 2 — SIMPLE MACHINES: ALL 6 TYPES + MECHANICAL ADVANTAGE The Six Simple Machines — Master Reference IMA (Ideal MA) = assumes no friction/energy loss. AMA (Actual MA) = F_out / F_in, measured in real world. AMA ≤ IMA always. Efficiency = AMA/IMA × 100% Machine IMA Formula Examples + Key Facts

LEVER IMA = d_effort / d_load Seesaw, crowbar, scissors. 3 classes

(see p.3).

INCLINED PLANE IMA = L / h L = slope length, h = vertical height.

Ramp/slide.

WEDGE IMA ≈ L / w L = wedge length, w = widest thickness.

Knife, axe, zipper.

WHEEL & AXLE IMA = R_wheel / R_axle Doorknob, steering wheel, screwdriver.

Radii matter.

PULLEY IMA = # of supporting

ropes

Fixed: changes direction only (IMA=1). Movable: IMA=2+.

SCREW IMA = 2πr / pitch Pitch = distance per one full turn. Bolt,

jar lid, drill.

1. Inclined Plane — Deep Dive A ramp. Allows you to move a load a longer distance with less force to reach the same height.

IMA (ramp) IMA = L / h^ L = length of slope, h = vertical rise

Force needed (ideal)

F_effort = (m·g·h) /

L

= Weight × (1/IMA) Weight components

W_∥ = mg·sin(θ) |

W_⊥ = mg·cos(θ)

Parallel (down slope) | Perpendicular (into surface) Example: Ramp 5 m long, 1 m high. IMA = 5/1 = 5. To lift 500 N load ideally takes only 100 N over 5 m. Trick: sin(θ) = h/L, cos(θ) = base/L. The steeper the ramp, the lower the IMA and the more force needed.

2. Wedge A moving inclined plane (or two back-to-back). Force applied to blunt end; output forces push outward/apart.

IMA (wedge) IMA = L / w^

L = wedge length (along slope), w = widest width Key point: A longer, thinner wedge = higher IMA = more splitting force for the same input. Examples: Knife blade, axe head, nail, zipper teeth, doorstop, plow blade, scalpel.

3. Screw An inclined plane wrapped around a cylinder. Each full rotation moves the screw one 'pitch' forward.

IMA (screw) IMA = 2π·r /^ pitch^

r = radius of handle/lever; pitch = advance per turn Pitch

pitch = 1 / (threads

per cm)

More threads per cm = smaller pitch = larger IMA Example: r = 0.1 m handle, pitch = 0.005 m → IMA = 2π(0.1)/0.005 = 125. Self-locking: Screws with small pitch angle won't move backward when effort is removed (friction ≥ component of load). Summary: Trade-Off Rule (The Golden Rule of Machines)

GAIN in Force →

Input distance > Output distance IMA > 1 (most common case) Example: Wheelbarrow, block & tackle

GAIN in Speed/Distance →

Output distance > Input distance IMA < 1 (sacrifices force for speed) Example: Tweezers, human forearm

KEY LAW: W_in = W_out (ideal) → F_in × d_in = F_out × d_out

Machines NEVER create energy — they only redirect or redistribute it.

EXAMPLE 1 — Find Effort Force 1st class lever. Load = 300 N at 0.5 m from fulcrum. Effort arm = 2.0 m. Find effort.

τ_load = τ_effort

300 × 0.5 = F_e × 2.

150 = 2F_e

F_e = 75 N

IMA = 2.0/0.5 = 4

EXAMPLE 2 — Find Fulcrum Position A 4 m lever. 800 N load on left end. 200 N effort on right end. Where is fulcrum?

Let x = dist from load to fulcrum

800·x = 200·(4−x)

800x = 800 − 200x

1000x = 800

x = 0.8 m from load end

Lever Device Tips (for the Practical Part)

  • Set up the lever on its fulcrum before adding any masses
  • Record the position of EACH mass carefully (measure from fulcrum, not from end)
  • Torque balance: m ·d₁ ₁ = m ·d₂ ₂(for two masses — set it and solve for unknowns)
  • With 3 masses: m d₁ ₁ + m d₂ ₂ = m d₃ ₃ (pick one side vs. the other)
  • Mass ratio = m /m₁ ₂ = d /d₂ ₁(the INVERSE of the distance ratio)
  • Use the balance point of the lever itself to determine its center of mass (mark it!)
  • When all torques balance and lever is level, you can solve for mass ratios directly

PAGE 4 — PULLEYS, WHEEL & AXLE, AND FORCE ANALYSIS Pulleys — Complete Guide A pulley is a wheel with a grooved rim where a rope/cable runs. Changes direction and/or magnitude of force. Type Characteristics IMA & Notes Fixed Pulley Axle is attached to a fixed support. Only changes direction of force — pull down to lift up. Like a flagpole.

IMA = 1 No force advantage; 1

rope supports load. Movable Pulley Axle moves WITH the load. Load is supported by 2 rope segments. Halves the effort needed.

IMA = 2 Must pull rope twice the

load's distance. Block & Tackle Combination of fixed and movable pulleys. Used in cranes, elevators, sailing. Many rope segments support the load.

IMA = # supporting rope

segments Count ropes holding the

movable block. How to Count Supporting Rope Segments RULE: Count ONLY the rope segments that are directly supporting the movable pulley/load block. Do NOT count:

  • The free end of the rope being pulled
  • Rope segments attached to a fixed support (these don't support the load) Example: 4 rope segments hold the lower (movable) block → IMA = 4. Effort = Load ÷ 4. You must pull 4× the distance the load rises. Pulley System Worked Examples Example A — effort needed A block & tackle has 5 supporting ropes. Load = 1000 N. η = 80%.

IMA = 5

AMA = η × IMA = 0.8 × 5 = 4

F_effort = Load / AMA = 1000/4 =

250 N

Example B — rope pulled IMA = 3 system. Load raised 2 m. How far is rope pulled?

d_input = IMA × d_output

d_input = 3 × 2 m = 6 m

You pull 6 m of rope to raise load 2 m. Wheel and Axle Two cylinders of different radii sharing the same axis of rotation. Effort applied to wheel; output at axle (or vice versa). IMA (effort on wheel)

IMA = R_wheel /

R_axle

R_wheel > R_axle → force multiplier IMA (effort on axle)

IMA = R_axle /

R_wheel

R_axle < R_wheel → IMA < 1 → speed multiplier

PAGE 5 — COMPOUND MACHINES, GEARS & EFFICIENCY Compound Machines A compound machine is two or more simple machines working together. Overall IMA = product of individual IMAs. Total IMA

IMA_total = IMA ₁ ×

IMA ₂ × IMA ₃ ...

Multiply IMA of every simple machine component Example: Lever IMA=3, pulley system IMA=4 → total IMA = 12 Common Compound Machines Machine Components How IMA Works

Scissors 2 levers + 2 wedges Two 1st-class levers sharing a fulcrum (the

screw). Blade edges act as wedges.

Wheelbarrow 2nd-class lever +

wheel & axle

Lever (handles) + wheel (rolls over ground reducing friction).

Bicycle Wheel/axle + gears +

levers (brakes)

Pedal crank → chain gear → rear wheel. Multiple gear ratios.

Crane Pulley system +

lever arm

Block & tackle × boom arm. Very high total IMA.

Stapler 2nd-class lever +

wedge

Pressing handle compresses spring, staple wedge pierces paper.

Axe on handle Lever + wedge Handle = 3rd-class lever; blade = wedge.

Jackscrew Screw + lever Turning a lever arm drives a screw. Used to lift

cars.

Drill press Wheel/axle + wedge +

screw

Motor → rotary motion → drill bit (wedge) + feed screw. Gears (Wheel & Axle Variant) Gears are interlocking toothed wheels. They transmit torque and can change speed, force, and direction of rotation. Gear Ratio (IMA)

IMA = T_output /

T_input

T = number of teeth on each gear Speed Relationship

ω_in / ω_out = T_out

/ T_in

ω = angular speed (rev/s or RPM) Torque Relationship

τ_out / τ_in = T_out

/ T_in

More output teeth = more output torque Direction Rule: Two meshing gears rotate in OPPOSITE directions. Add an idler gear between them → same direction.

Gear Train Analysis FORCE Advantage (Speed Reducer) Small input gear → Large output gear

T_in = 10, T_out = 50

IMA = 50/10 = 5

Output torque = 5× input torque Output speed = 1/5 input speed Example: Car low gear, wrench socket drive SPEED Advantage (Torque Reducer) Large input gear → Small output gear

T_in = 60, T_out = 20

IMA = 20/60 = 0.

Output speed = 3× input speed Output torque = 1/3 input torque Example: Bicycle high gear, fan/propeller Efficiency Efficiency measures how much of the input work actually becomes useful output work. Always ≤ 100% due to friction. Efficiency

η = (W_out / W_in) ×

W in Joules; η as percentage (0–100%) Also

η = (AMA / IMA) ×

AMA = actual, IMA = ideal (no friction) Work Output

W_out = F_load ×

d_load

Useful work done on the load Work Input

W_in = F_effort ×

d_effort

Work done by you on the machine Energy Lost (heat)

W_friction = W_in −

W_out

Energy that went to heat/sound Example: Efficiency Calculation A ramp (IMA=4) is used to push 200 N box up a 4 m slope. Effort = 60 N.

W_in = 60 N × 4 m = 240 J

h = 4/4 = 1 m (since IMA = L/h)

W_out = 200 N × 1 m = 200 J

η = 200/240 × 100% = 83.3%

Key Efficiency Facts

  • η = 100% only in ideal (frictionless) machines
  • η < 100% always in real life
  • Higher friction → lower η
  • AMA < IMA when η < 100%
  • Lubrication increases η
  • Smooth surfaces increase η Comparing IMA vs AMA IMA (Ideal Mech. Advantage) AMA (Actual Mech. Advantage) Based ONLY on geometry/measurements Based on measured forces: F_out / F_in No friction assumed Includes friction and losses = d_input / d_output = F_output / F_input

PAGE 6 — ENERGY, MOMENTUM, CIRCULAR MOTION & EXAM TIPS Energy Conservation & Machines The Law: Energy cannot be created or destroyed, only transformed. Total mechanical energy = KE + PE. Mechanical Energy

E_mech = KE + PE =

½mv² + mgh

Conserved when no friction With friction

E_mech,f = E_mech,i

− W_friction

W_friction = f_k × d (energy lost to heat) Ramp launch

mgh = ½mv² → v =

√(2gh)

Object sliding down frictionless ramp from height h

On an inclined plane with friction: KE_bottom = mgh − μ_k·mg·cos(θ)·L

Momentum & Impulse Momentum describes how hard it is to stop a moving object. Impulse is the change in momentum.

Momentum p = m·v^ kg·m/s — vector quantity (has direction)

Impulse J = F·Δt = Δp^

Larger time → smaller force for same Δp (e.g., airbag) Conservation of Momentum

m ₁ ₁ v + m ₂ ₂ v = m ₁ ₁ v '

+ m ₂ ₂ v '

Total momentum constant when no external forces Elastic collision

KE conserved:

½m ₁ ₁ v ²+½m ₂ ₂ v ² =

½m ₁ ₁ v '²+½m ₂ ₂ v '²

Billiard balls, ideal collisions Perfectly Inelastic

(m ₁ +m ₂ )v_f = m ₁ ₁ v +

m ₂ ₂ v

Objects stick together after collision Circular Motion & Centripetal Force Centripetal force is the net inward force required to keep an object moving in a circle. It is NOT a separate force — it's the label for whatever force (tension, gravity, normal, friction) points toward the center. Centripetal Force

F_c = m·v²/r =

m·ω²·r

Always points toward center of circle

Centripetal Acceleration a_c = v²/r^ m/s² — directed inward

Period T = 2πr/v =^ 2π/ω^ Time for one full revolution; ω in rad/s

Angular velocity ω = 2π/T = 2πf^ Radians per second; f = frequency in Hz

On a banked curve: tan(θ) = v²/(r·g) — no friction needed at this exact speed

Vertical circle (top): F_c = mg + N (or T) — gravity adds to centripetal force at top

Inertia & Rotational Inertia

Inertia I ∝ m (linear)^ More mass = harder to accelerate

Rotational Inertia (Moment of Inertia)

I = Σmr² Depends on mass distribution and axis

Point mass on rod I = mr²^ r = distance from rotation axis

Newton's 2nd (rotation) τ_net = I·α^ α = angular acceleration; analogous to F=ma

All Formulas Quick-Reference Card MECHANICS SIMPLE MACHINES ENERGY / MOMENTUM

F = ma

W = Fd·cos(θ)

v = v ₀ + at

Δx = v ₀ t + ½at²

v² = v ₀ ² + 2aΔx

τ = F·d_⊥

F_c = mv²/r

f_k = μ_k·N

N = mg (flat)

IMA = d_in/d_out

AMA = F_out/F_in

η = AMA/IMA × 100%

Lever: IMA=d_e/d_L

Ramp: IMA=L/h

Pulley: IMA=# ropes

W&A: IMA=R_w/R_a

Screw: IMA=2πr/p

Gears: IMA=T_out/T_in

KE = ½mv²

PE = mgh

W_net = ΔKE

p = mv

J = FΔt = Δp

P = W/t = F·v

ω = 2π/T

τ_net = Iα

v = √(2gh)

Exam Strategy & Common Mistakes ⚠ COMMON MISTAKES

  • Forgetting to label units — ALWAYS write N, m, J, etc.
  • Confusing IMA and AMA — IMA uses distances, AMA uses forces
  • Wrong lever class — always identify position of fulcrum, effort, load
  • Counting wrong rope segments in

✅ WINNING TIPS

  • Draw a diagram and FBD for EVERY problem
  • For levers: ALWAYS use torque balance about the fulcrum
  • For pulleys: count supporting ropes, then multiply effort by IMA = distance you pull
  • For efficiency: check if η < 100% before