ContentsThe library

Waves, Modes and Frequency

Pushing at the Rate a Thing Already Has

Last timeA Shape That Moves While Nothing Travels With It

Push an oscillator at its own rate and small pushes accumulate into a large swing. The response is sharp or blunt depending on how fast the system loses what it is given.

A child on a swing is pushed gently and ends up going high. Nothing about any one

push explains the result, because the pushes are small and the swing is large. What

explains it is their timing.

FIG 1An oscillator with a push and a leak
the restoring pull proportional to displacement, which is what makes this an oscillator and was the whole of the first lesson
the leak: a resistance proportional to speed, which removes energy from the motion. Without it nothing in this lesson has a finite answer
the push, applied at a rate the pusher chooses rather than one the system has. The whole question is what happens as that chosen rate is varied
the rate of pushing. This is the number along the bottom of the figure below, and the system's own rate is a separate number entirely
Every term in this has appeared before except the two new ones. The first lesson of the course had the first and the last. The middle term on the left is the leak, and the right-hand side is the push. Those two additions are the entire subject of this lesson, and between them they decide both how large the response is and how fussy the system is about the rate it is given.

The response, and what the leak does to it

Push at a rate well below the system's own and it simply follows the push, with a

small swing. Push far above and it cannot keep up, and the swing is smaller still.

Push at its own rate and the pushes arrive in step with the motion that is already

there, each one adding to it, and the swing becomes large.

FIG 2How big a swing, as the pushing rate is varied
024681000.511.522.5pushing rate, as a multiple of the system's own rate
size of the steady swing
Drag the leak from small to large and watch the two things that change together. With a small leak the peak is tall and extremely narrow: this system answers one rate and almost nothing else. With a large leak the peak is low and broad, and the system responds moderately to a wide range of rates. There is no setting that gives a tall broad peak, because the height and the width are controlled by the same number.

That is worth stating as a trade rather than as two facts. A system that holds on to

energy builds up an enormous response, but only when the rate is almost exactly

right, because the long memory lets a small mismatch accumulate into opposition. A

system that loses energy quickly cannot tell a slightly wrong rate from the right

one, because it has forgotten the earlier pushes by the time the mismatch would have

mattered.

The lesson stops here

5 more paragraphs to go

You have read the opening. The rest of the argument, the problems that check whether it landed, and the lines worth keeping at the end all come with a plan.

The first lesson of every course in the library reads the whole way through, free, so you can see exactly what the rest of them are.

See the planThe contents

This is the reading half

Starting the course gives you your own copy of it. Every idea on every page has problems standing under it, marked with a reason rather than a tick, and any sentence you do not believe can be opened and argued with. None of that can happen on a page nobody owns.

The contents

The rest of this course

  1. 01The One Rhythm Nearly Everything Falls Into
  2. 02Two Joined Pendulums and the Two Rhythms Hiding in Themopening only
  3. 03What a Clamped String Is Allowed to Doopening only
  4. 04Every Starting Shape Is a Sum of the Allowed Onesopening only
  5. 05A Travelling Wave Is Two Standing Onesopening only
  6. 06Pushing at the Rate a Thing Already Hasyou are here
  7. 07The Ring That Forgetsopening only
  8. 08Charges, Loops and a Wave With Nothing to Waveopening only

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