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Engineering

Marine chronometer and navigation

Keep time at sea by lamplight: a balance wheel on its hairspring, kicked once a beat by a detent escapement, beats seconds in a gimballed box. Warm the cabin and watch an uncompensated balance lose two minutes a day, then let the bimetal rim take the linear error out and leave the small middle-temperature error; lock the gimbals in a heeled box and an out-of-poise balance gains or loses with its amplitude, almost not at all near 220 degrees; set the voyage length and read how far east or west a navigator would place the ship. The impulses given are booked against every loss.

Marine chronometer and navigation — Actual application image
Actual application image

What happens

A balance wheel of 8 g and 22 mm radius on its hairspring beats once a second; a detent escapement gives it a fixed impulse of 36 µJ exactly at the upward zero crossing, located inside the step by a cubic Hermite refined by Newton, against air drag and pivot friction. Temperature softens the hairspring and swells the rim; the bimetal rim’s compensation removes the linear part and leaves the middle-temperature error. With the gimbals locked in a heeled box an out-of-poise balance feels a gravity torque. RK4 at 1 ms; the rate in seconds a day comes from the crossings, the closed form from the exact Duffing period, the poise term 2 J1(A)/A and the viscous shift.

Try this

Read the baseline rate, then warm the cabin with and without compensation; lock the gimbals, heel the box and put the balance out of poise at different amplitudes; set the voyage and read the error of longitude.

The model and its limits

A rigid balance on a linear hairspring with a cubic isochronism term, an instantaneous detent impulse, lumped drag and friction, a quadratic temperature law. Rates are those of this idealized movement, not of any maker’s chronometer.

Equations used in the module
Equations
I(T)·α = −k(T)·θ·(1 + ε·θ²) − c·ω − τ_f·tanh(ω/ω_f) − m·g·e·sin φ·sin θ
k(T) = k0·(1 + α_s·ΔT),  I(T) = I0·(1 + (α_r − κ·(α_r − α_s))·ΔT + κ·β·ΔT²)
ω+ = √(ω² + 2E_i/I) at θ = 0,  E_i = π·c·ω·A² + 4τ_f·A
rate = 86400·(T_ref/T − 1),  Δλ = rate·days/240

Related experiments

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Phonograph: sound in a groove — Actual application image

Engineering

Phonograph: sound in a groove

Play a wax cylinder in a lamp-lit parlour: the hill-and-dale groove lifts a stylus tip that drives the mica diaphragm through its lever spring, and the horn turns the diaphragm’s motion into sound. Watch the groove magnified two thousand times beside the machine and the stylus riding it; raise the tone past the closed-form mistracking frequency and the tip flies off the hills; speed the cylinder up and the pitch rises in proportion; load the diaphragm with a better horn and it radiates more. The groove work is booked against every loss and the sound radiated.