Simple Machines – Comprehensive Study Notes

Page 1 — Objectives

  • After completing the chapter, students will be able to:

    • Describe the different types of machines (simple & compound).

    • Explain and use the terms Mechanical Advantage (MA), Velocity Ratio (VR), efficiency (η) and other related quantities.

    • Solve numerical problems based on MA, VR and efficiency.

    • Describe the concept of moment (torque) and its effects.

    • Vr, MA and effiency


Page 2 — Visual Overview of Simple Machines

  • Historical banner: “40 Years of Academic Excellence (1904-2004)” – GEMS Cambridge International School.

  • Infographic shows the six classical simple machines:

    1. Lever – labelled with fulcrum, load & effort.

    2. Inclined Plane – shows force applied along slope to raise load.

    3. Pulley – wheel with groove; rope lifts load.

    4. Wheel & Axle – large wheel paired with smaller axle to multiply force or speed.

    5. Wedge – double-inclined plane used for splitting/cutting.

    6. Screw – inclined plane wrapped helically around a shaft.

  • Purpose of graphic: immediate recognition of each simple machine and its force-load relationship.


Page 3 — Introduction to Machines

  • Definition: A machine is a device that makes human work easier, faster and more convenient.

  • Four principal ways a machine helps:

    1. Changing direction of applied effort (e.g., flagpole pulley).

    2. Multiplying effort (magnifying force) so a small effort lifts a heavy load (e.g., jack screw).

    3. Increasing speed (sacrificing force for velocity, e.g., bicycle gear).

    4. Improving safety (isolating user from danger, providing stable posture, etc.).


Page 4 — Key Terminology (Part 1)

  • Effort (E): Force applied to the machine in order to overcome load.

  • Load (L): Resistive force lifted or overcome by the machine.

  • Fulcrum (F): Fixed point about which a lever or rotating part pivots.

  • Effort Arm (EDED): Perpendicular distance from fulcrum to the point of effort application.


Page 5 — Key Terminology (Part 2)

  • Load Arm (LDLD): Perpendicular distance from fulcrum to the point where the load acts.

  • Input Work (Win): Work done on the machine.
    W</em>in=E×EDW</em>{in}=E \times ED

  • Output Work (Wout): Work done by the machine.
    W</em>out=L×LDW</em>{out}=L \times LD


Page 6 — Principle of a Perfect Machine + Mechanical Advantage

  • Principle of Machine: In a perfect (friction-less) machine,
    W<em>in=W</em>out    E×ED=L×LDW<em>{in}=W</em>{out}\;\Longrightarrow\; E \times ED = L \times LD

  • Mechanical Advantage (MA): Ratio of load overcome to effort applied.
    MA=LEMA = \frac{L}{E}
    • Unit-less (ratio of forces).
    Affected by friction: High friction ↓ MA.


Page 7 — Velocity Ratio & Efficiency

  • Velocity Ratio (VR): Ratio of velocity/distance moved by effort to that moved by load.
    VR=Effort distanceLoad distanceVR = \frac{\text{Effort distance}}{\text{Load distance}}
    Independent of friction (purely geometrical).

  • Efficiency (η): Fraction of input work converted to useful output work.
    η=W<em>outW</em>in×100%\eta = \frac{W<em>{out}}{W</em>{in}} \times 100\%
    η=MAVR×100%\eta = \frac{MA}{VR} \times 100\%
    • Practical machines have \eta < 100\% due to friction & self-weight.


Page 8 — Six Classical Simple Machines

  1. Lever

  2. Pulley

  3. Wheel & Axle

  4. Inclined Plane

  5. Wedge

  6. Screw


Page 9 — Pulley: Definition

  • Pulley: Circular metallic/wooden disc with a grooved rim that rotates about a central axle.

  • Function: Changes direction of force and/or multiplies effort depending on configuration.


Page 10 — Pulley Types Overview

  1. Fixed Pulley

    • MA ≈ 1 (ideal).

    • Changes direction only.

  2. Movable Pulley

    • MA ≈ 2 (ideal).

    • Magnifies effort; does not change direction.

  3. Pulley System (Block & Tackle)

    • MA equals the number of rope segments supporting load (ideal).

Illustrations show ceiling-mounted fixed pulley, hand supplying effort, etc.


Page 11 — Single Fixed Pulley (Details)

  • Rope passes over fixed pulley; load on one end, effort on the other.

  • Effort distance = load distance ⇒ VR=1VR=1.

  • Purpose: Only changes direction so we can pull downward to lift load upward.

Formulas for ideal fixed pulley:
MA=1,  VR=1,  η=MAVR=100%  (theoretical)MA=1,\; VR=1,\; \eta=\frac{MA}{VR}=100\%\;\text{(theoretical)}


Page 12 — Single Movable Pulley

  • Pulley attached to load; rope anchored at one end, effort applied on free end.

  • Two rope segments share the load.
    VR=2VR = 2 (Effort travels twice load distance).

  • Advantages: Effort is halved (ideal). Direction not changed.


Page 13 — Combined Pulley (Block & Tackle)

  • Two blocks: upper (fixed) & lower (movable) each containing multiple pulleys.

  • Rope woven alternately between blocks.

  • Provides both direction change and effort magnification.

  • Ideal rule:
    VR=Number of pulleys=Number of supporting rope segmentsVR = \text{Number of pulleys} = \text{Number of supporting rope segments}


Page 14 — General VR Expression for Pulleys

VR=Effort distanceLoad distance=No. of pulleys (or rope segments supporting load)VR = \frac{\text{Effort distance}}{\text{Load distance}} = \text{No. of pulleys (or rope segments supporting load)}


Page 15 — Numerical 1 (Worked Example)

Problem:
• A single movable pulley has efficiency η=75%\eta = 75\%.
• Load L=500NL=500\,\text{N}.
Find the required effort $E$.

Solution Outline:

  1. Ideal MA for one movable pulley: MAideal=2MA_{ideal}=2.

  2. Actual MA: MAactual=η×VR100=0.75×2=1.5MA_{actual}= \eta \times \frac{VR}{100} = 0.75 \times 2 = 1.5.

  3. Compute effort:
    E=LMAactual=5001.5=333.3NE=\frac{L}{MA_{actual}}=\frac{500}{1.5}=333.3\,\text{N}


Page 16 — Numerical 2 (Four-Pulley System)

Given:
• Four-pulley block & tackle, η=80%\eta=80\%, L=1800NL=1800\,\text{N}, load raised 6m6\,\text{m}.

(a) MA<em>ideal=VR=4MA<em>{ideal}=VR=4 (four supporting segments). MA</em>actual=η×VR100=0.80×4=3.2MA</em>{actual}=\eta \times \frac{VR}{100}=0.80\times4=3.2

(b) Effort:
E=LMAactual=18003.2=562.5NE=\frac{L}{MA_{actual}}=\frac{1800}{3.2}=562.5\,\text{N}

(c) Output work:
Wout=L×h=1800×6=10800JW_{out}=L \times h = 1800 \times 6 = 10800\,\text{J}

(d) Input work:
W<em>in=W</em>outη=108000.80=13500JW<em>{in}=\frac{W</em>{out}}{\eta}=\frac{10800}{0.80}=13500\,\text{J}


Page 17 — Numerical 3 (Unknown Pulleys)

Given: η=80%\eta=80\%, MAactual=4MA_{actual}=4, L=1000NL=1000\,\text{N}.

  1. Determine ideal VR:
    η=MA<em>actualVR×100%    VR=MA</em>actualη/100=40.8=5\eta=\frac{MA<em>{actual}}{VR} \times 100\% \;\Longrightarrow\; VR=\frac{MA</em>{actual}}{\eta/100}=\frac{4}{0.8}=5
    ⇒ Five supporting rope segments ⇒ 5 pulleys (assuming standard arrangement).

  2. Effort:
    E=LMAactual=10004=250NE=\frac{L}{MA_{actual}}=\frac{1000}{4}=250\,\text{N}


Page 18 — Wheel & Axle: Description & Theory

  • Consists of two coaxial cylinders: large wheel radius RR, small axle radius rr (R > r).

  • Effort applied at wheel rim, load lifted at axle via rope.

  • Acts as a continuous first-class lever (fulcrum at axle bearing).

  • Ideal relations:
    VR=Effort distance per turnLoad distance per turn=2πR2πr=RrVR = \frac{\text{Effort distance per turn}}{\text{Load distance per turn}} = \frac{2\pi R}{2\pi r} = \frac{R}{r}
    MAideal=VRMA_{ideal}=VR

  • Examples: Screwdriver, doorknob, steering wheel, sewing-machine balance wheel.


Page 20 — Wheel & Axle Numerical

Data: R=40cm=0.40m,  r=0.1m,  L=1200N,  E=400N,  load rise=4mR = 40\,\text{cm}=0.40\,\text{m},\; r=0.1\,\text{m},\; L=1200\,\text{N},\; E=400\,\text{N},\; \text{load rise}=4\,\text{m}

(a) MA=LE=1200400=3MA = \frac{L}{E} = \frac{1200}{400}=3
(b) VR=Rr=0.400.10=4VR = \frac{R}{r} = \frac{0.40}{0.10}=4
(c) η=MAVR×100%=34×100%=75%\eta = \frac{MA}{VR}\times100\% = \frac{3}{4}\times100\% = 75\%
(d) Output work: W<em>out=L×h=1200×4=4800JW<em>{out}=L\times h = 1200 \times 4 = 4800\,\text{J} (e) Input work: W</em>in=Woutη=48000.75=6400JW</em>{in}=\frac{W_{out}}{\eta}=\frac{4800}{0.75}=6400\,\text{J}


Page 21 — Inclined Plane: Fundamentals

  • Rigid flat surface set at angle θ\theta to horizontal.

  • Enables heavy loads to be raised with smaller effort along slope.

  • Everyday examples: mountain roads, staircases, planks into trucks.


Page 22 — Inclined Plane Formulae

VR=Effort distanceLoad distance=Length of plane (l)Height (h)=lhVR = \frac{\text{Effort distance}}{\text{Load distance}} = \frac{\text{Length of plane }(l)}{\text{Height }(h)} = \frac{l}{h}

If neglecting friction: MAideal=VRMA_{ideal}=VR.


Page 23 — Inclined Plane Numerical Example

Given: l=16m,  h=5m,  L=850N,  E=340Nl=16\,\text{m},\; h=5\,\text{m},\; L=850\,\text{N},\; E=340\,\text{N}

  • MA=LE=850340=2.5MA=\frac{L}{E}=\frac{850}{340}=2.5

  • VR=lh=165=3.2VR=\frac{l}{h}=\frac{16}{5}=3.2

  • η=MAVR×100%=2.53.2×100%=78.12%\eta=\frac{MA}{VR}\times100\%=\frac{2.5}{3.2}\times100\%=78.12\%

  • Output work (load raised vertical distance hh):
    Wout=L×h=850×5=4250JW_{out}=L\times h = 850\times5=4250\,\text{J}


Page 24 — Screw: Structure & Uses

  • Screw = cylindrical shaft with helical inclined plane (thread).

  • Converts rotational motion → linear motion.

  • Common applications: fasteners (furniture, electronics), screw jacks (lifting cars), micrometers (precise adjustment), orthopedic bone fixation.


Page 25 — Screw Velocity Ratio

For one full turn of handle:
VR=2πrpVR = \frac{2\pi r}{p}
Where:
rr = radius of lever/handle.
pp = pitch (axial distance between adjacent threads).

Higher VR ⇒ greater force multiplication (but greater turns for same lift).


Page 26 — Wedge

  • Formed by two joined inclined planes meeting at sharp edge.

  • Converts effort along length into forces normal to surfaces – splits or lifts material.

  • Uses: log-splitters, axe blades, chisels, knives, doorstops.

  • Velocity Ratio:
    VR=Length of wedge (l)Thickness / width (w)VR = \frac{\text{Length of wedge }(l)}{\text{Thickness / width }(w)}


Page 27 — Compound Machines

  • Compound Machine: Device combining two or more simple machines for greater overall MA.

  • Each component contributes to total performance.

  • Examples:
    Bicycle – levers (brakes), wheel & axle (wheels), pulleys (chain & gears).
    Scissors – double lever + wedge blades.
    Wheelbarrow – lever handles + wheel & axle wheel.
    Can Opener – levers, wedges, wheel & axle.

Ethical/Practical Insight: Compound machines reflect engineering optimisation—balancing force, speed, cost & safety to meet human needs effectively.


Cross-connections & Broader Context

  • All simple machines obey energy conservation: regardless of MA, the product (force × distance) remains (ideally) constant—larger force over shorter distance or vice versa.

  • Friction and material strength are the real-world constraints lowering efficiency.

  • Moments (torque) underpin lever, wheel & axle, and pulley operation: τ=F×d\tau = F \times d.

  • Understanding simple machines lays groundwork for analysing complex mechanical systems, robotics, biomechanics and everyday tools.