Civilization101Blueprint

Engineering

Turning the sciences into things that work: machines, structures, water in pipes and channels, heat through walls, and feedback control. Each result with what it lets you do and who first found it.

Home: Production, Level 4 · Engine, level 1 of 1 in its track. Serves 11 steps across 5 subjects.

Engineering is science with a safety factor. A plank on edge is 16 times stiffer than the same plank laid flat; three turns of rope round a post let one hand hold a pull of a quarter of a tonne; a pipe one size larger loses 70 % less of its pressure to friction; ten parts each 99 % reliable make a machine that works only 90 % of the time.

This page gives the results in the order each needs the last: forces and machines, structures, water in pipes and channels, heat, and control, then what has changed since 2000. The properties of the materials are in materials data; the physics underneath is on physics.

At a glance: what builds on what

Each part uses the ones above it.

PartResultsWhat depends on it
1 · Forces and machinesLevers and pulleys, friction and the capstanLifting, hauling, mooring, gears and belts
2 · StructuresStress and strain, beams, columnsHouses, barns, bridges, frames, towers
3 · WaterPipe friction, open channels, water powerWater supply, irrigation, drainage, mills, pumps
4 · HeatHeat through walls, how things coolInsulation, cold stores, food safety, kilns
5 · ControlFeedback, and reliabilityGovernors, thermostats, autopilots, any machine that must not fail
6 · Since 2000Cheap solar power, the tallest structuresWhat is now possible

Part 1Forces and machines

Levers, pulleys and the capstan

No machine gives out more work than is put in. What a machine does is trade force for distance, or use friction to hold a load.

Levers, pulleys and gears
F1d1=F2d2,MA=FoutFin

Ignoring friction, the force times the distance it moves is the same at both ends of a lever, a pulley system or a gear train. A block and tackle with four ropes supporting the load lifts it with a quarter of the pull, over four times the length of rope; a gear with three times the teeth turns a third as fast with three times the torque.

Use: Lifting stone, timber and engines without a crane; sizing a mill's gearing to its millstone (woodworking and the first machines). Friction takes 5–10 % per pulley in practice, so add a margin.

First: Archimedes' law of the lever, about 250 BC (MacTutor).

Friction and the capstan equation
F≤μN,Tload=Tholdeμθ

Friction can resist up to μ times the force pressing two surfaces together. Rope wrapped round a post multiplies this exponentially with the angle of wrap θ in radians. With μ = 0.3, three full turns (θ = 6π) hold a load about 285 times the holding pull.

Use: Snubbing a boat or a falling tree round a post, lowering loads, belaying: a few turns let one person hold what no person could lift (knots). It also sets how much a belt can drive before it slips.

First: Euler, 1760s (MacTutor); Amontons's laws of friction, 1699.

A trucker's hitch: a loop in the standing part acts as a pulley, roughly doubling the pull to tension a load or a ridgeline. Hitch-truckers-ABoK 1514-USCG · 2020-01-30 05:43:43 · USCG PTC Developer · CC BY-SA 4.0 · Commons ↗
The great brake wheel inside Bembridge mill, Isle of Wight: wooden cogs on a wheel keyed to the windshaft, with the brake band round its rim. One wheel takes all the sails' power, and stopping it is the only brake the mill has. Bembridge Windmill, Great brake wheel - geograph.org.uk - 6243364 · 2019-08-17 · Michael Garlick · CC BY-SA 2.0 · Commons ↗

Part 2Structures

Stress, beams and columns

A structure fails when the stress somewhere in it passes what its material can bear, or when a slender part buckles sideways first. Design for several times the largest load expected: a safety factor of 2–4 for steel, more for timber and masonry, whose strength varies more.

Stress, strain and the safety factor
σ=FA,σ=Eε,n=σfailσworking

Stress σ is force per area, in pascals; strain ε is the stretch per length. Below its limit a material stretches in proportion, by its stiffness E: 200 GPa for steel, about 10–15 for timber along the grain. Mild steel yields at about 250 MPa.

Use: A 10 mm steel rod (78.5 mm²) yields at about 20 kN, two tonnes; at a safety factor of 4 it should carry half a tonne. The same sums size bolts, chains, hangers and rope.

First: Hooke's law, 1678 (MacTutor); Thomas Young's modulus, 1807 (MacTutor).

Beams
σmax=McI,I=bh312Mmax=wL28,δ=5wL4384EI

A beam carrying w per metre over a span L bends with a moment greatest at mid-span; the stress is highest at its top and bottom faces, a distance c from the middle. Its resistance to bending, I, grows with the cube of its depth h. Sag grows with the fourth power of the span.

Use: A 50 × 200 mm joist on edge is 16 times stiffer and 4 times stronger than laid flat. Doubling a span with the same beam quadruples the stress and multiplies the sag by 16: use more, deeper joists, or a post at mid-span (framed building).

First: Galileo's first theory of beam strength, Two New Sciences, 1638 (MacTutor); the bending theory of Euler and Daniel Bernoulli, 1744–1750; Navier put the neutral axis right, 1826 (MacTutor).

Columns: Euler buckling
Pcr=π2EI(KL)2

A slender post or strut fails by bowing sideways at the critical load, long before the material crushes. The load falls with the square of the effective length K L: K is 1 with both ends pinned, 0.5 with both fixed, 2 for a flagpole free at the top.

Use: Halving a post's free length, by a brace at mid-height, quadruples the load it can carry; a fat hollow tube beats a thin solid bar of the same weight. Why scaffolds, towers and frames are braced diagonally (iron-framed building).

First: Leonhard Euler, 1744 (MacTutor).

Raising a timber-frame bent, 2008: posts, tie beam, rafters and diagonal knee braces joined flat on the ground, then lifted and stood up as one piece. Large Flying Bent · 12/29/08 · Vermont Timber Works Inc. · CC BY-SA 3.0 · Commons ↗
A cast-iron column at Immenstadt station, Germany (2025): riveted iron beams bear on its capital, and the column carries their load straight down in compression. Bhf Immenstadt - Kapitell Gleis 1 - 2025-06-10 - 164c · 2025-06-10 · Martinus KE · CC BY-SA 4.0 · Commons ↗

Part 3Water

Pipes, channels and water power

Moving water loses energy to friction in proportion to the square of its speed; falling water gives energy in proportion to its height. The three results here size a water main, a ditch and a mill.

Friction in pipes: Darcy–Weisbach
hf=fLDv22g,Re=ρvDμ

Flow through a pipe of length L and bore D at speed v loses a head of water set by the friction factor f. Below a Reynolds number of about 2,000 the flow is smooth and f = 64/Re; above about 4,000 it is turbulent and f is about 0.015–0.03, read from the Moody chart.

Use: At a fixed flow, head loss falls with the fifth power of the bore: a 32 mm pipe loses about 70 % less than a 25 mm one carrying the same water. Size mains and irrigation lines so the loss leaves enough pressure at the far end (irrigation).

First: Weisbach, 1845 (MacTutor), and Darcy, 1857; Reynolds found the change from smooth to turbulent flow, 1883 (Philosophical Transactions); Moody's chart, 1944 (Transactions of the ASME).

Open channels: Manning's equation
v=1nRh2/3S1/2

Water in a ditch, canal or gutter flows at a speed set by its hydraulic radius (flow area divided by wetted perimeter), the slope S and the roughness n: about 0.013 for smooth concrete, 0.02–0.03 for clean earth, more for weeds and stones.

Use: An earth ditch 1 m wide running 0.5 m deep on a slope of 1 in 1,000, with n = 0.025, moves about 0.5 m/s, 250 litres a second. Keep speeds between about 0.3 m/s (silting) and 1 m/s (scour in earth) (canals and locks).

First: Gauckler, 1867, and Manning, 1891; roughness values from the US Geological Survey (Arcement and Schneider, 1989).

Water power
P=ηρgQH

The power in a flow Q (m³/s) falling a head H is ρ g Q H; a machine converts a fraction η of it: about 0.6–0.7 for a good water wheel, 0.8–0.9 for a turbine. Pumping needs the same power the other way, divided by the pump's efficiency.

Use: A stream of 50 litres a second falling 10 m holds 4.9 kW; a wheel delivers about 3 kW (water power). Lifting 1 litre a second 20 m takes 196 W of water power, about 400 W from a small pump.

First: John Smeaton's model experiments on water wheels, 1759 (Philosophical Transactions).

The head of a drip system in Kerala, India (2022): PVC pipe with valves feeds the drip laterals laid along the crop rows. Drip irrigation in Kerala · 2022-09-01 16:42:28 · Vis M · CC BY-SA 4.0 · Commons ↗

Part 4Heat

Heat through walls, and how things cool

Heat moves by conduction through solids, convection in air and water, and radiation. For a building, a cold store or a pot of food, two results do most of the work.

Heat through a wall
Q=UAΔT,U=1∑t/k

Heat flow Q through an area A is its U-value times the temperature difference. Each layer resists in proportion to its thickness t over its conductivity k: about 0.035–0.04 W/(m K) for mineral wool or sheep's wool, about 0.06 for straw, 0.6–1.0 for brick, 1.5–2 for concrete, 1 for glass and 50 for steel.

Use: 100 mm of wool (U about 0.35) loses a sixth of the heat of a solid brick wall (U about 2); a single pane loses about four times as much as good double glazing. Insulate the roof first, where warm air collects (plan the house).

First: Joseph Fourier, Théorie analytique de la chaleur, 1822 (MacTutor).

Newton's law of cooling
T(t)=T∞+(T0−T∞)e−t/τ,τ=mchA

A body cools toward its surroundings exponentially, with a time constant τ set by its heat capacity over its surface area and the heat-transfer coefficient h. Water draws heat away many times faster than still air at the same temperature.

Use: Food cools through the danger zone fast enough only in shallow layers: divide a deep pot of stew into trays about 5 cm deep before chilling (biology: bacteria double). The same law times quenching in smithing, and explains why a person in cold water chills far faster than in cold air.

First: Isaac Newton, Scala graduum caloris, 1701 (Philosophical Transactions).

Part 5Control

Feedback, and reliability

Reliability multiplies. Parts in series must all work, so their reliabilities multiply: ten parts each 99 % reliable make a machine 90 % reliable. Parts in parallel fail only together: two pumps each available 90 % of the time give water 99 % of the time. Spares and redundancy buy more than better parts.

Feedback control: proportional, integral, derivative
u(t)=Kpe(t)+Ki∫0tedτ+Kddedt

A controller measures the error e between what is wanted and what is, and acts in proportion to it, to its accumulated total, and to its rate of change. Too much proportional gain makes the system hunt and oscillate; the integral term removes a steady offset; the derivative damps overshoot.

Use: The centrifugal governor on an engine or mill, a thermostat, a float valve, an autopilot and a kiln controller are all this loop. Tune by raising the proportional gain until it just starts to oscillate, then back off (the factory).

First: Maxwell analysed the stability of governors, 1868 (Proceedings of the Royal Society); Minorsky's three-term controller for steering ships, 1922 (Journal of the American Society for Naval Engineers).

Part 6Since 2000

What has changed since 2000

Each line is from its primary source.

ResultYearWhat it changedSource
Solar the cheapest new power2010–2023The average cost of electricity from new utility-scale solar fell by 90 %, to US$0.044 per kWhIRENA
Cheap storage1991–Lithium-ion cells fell about 97 % in priceChemistry since 2000
The tallest structure2010Burj Khalifa, Dubai, 828 m: a buttressed concrete core resisting wind as much as weightSkyscraper Center

Where to go next

This page covers what you are most likely to meet. It is not a field guide, and on identification that difference can kill you. These are the works that go further — chosen because they can be held offline.