In the main series we peeled force all the way apart. In the bonus we chase the deep kinship between force and "waves"
Over the 12 episodes of the main series, we peeled the true nature of force back to relationship, geometry, gauge, and curvature. In the bonus we shift our gaze a little and, over three installments, chase the kinship between force and "waves." Waves ── a vibrating string, sound, the water's surface, light ── feel as if there's some independent "wave stuff" out there. But there isn't. The first installment takes the most naive direction: how, exactly, is a wave born from force? The answer is almost anticlimactically simple, and it's built entirely from the tools we made in the main series (spring = restoring force, and inertia). A wave turned out to be a game of "telephone" in force ── each neighbor pushing the next.
String a lot of little weights (masses) together with springs, like beads on a chain. Flick one weight sideways ── what happens? As we saw in Episode 3, the spring pulls its neighbor with a restoring force that tries to snap things back. The neighbor, being pulled, doesn't move right away ── because of the inertia from Episode 1, it starts moving a little late. Once it moves, it pulls the next neighbor in turn ── and this chain of "pull (force) → move a beat later (inertia) → pull the next" travels from end to end. That is a wave.
Restoring force (the force pulling a neighbor back, Episode 3) + inertia (can't move instantly, Episode 1).
Line these two up across space, and a single wiggle gets passed along with a delay, "to the neighbor, and the next."
A wave is not an independent entity; it's the phenomenon of a chain of force and inertia propagating.
So how fast does the message travel? Two tugs-of-war decide it ── the stronger the restoring force, the quicker it yanks the neighbor, so faster. The larger the inertia (weight), the more sluggish the start, so slower. For a string, the restoring force is the tension \(T\) and the inertia is the linear density \(\mu\) (the weight per meter). Written out, it's just \(F=ma\) (Episode 1) applied to the chain, and it comes out like this.
Tighten a guitar string (large \(T\)) and the pitch rises (the wave is faster). A thick string (large \(\mu\)) is low (the wave is slower) ── exactly as this formula says. The speed of a wave is set by the ratio of force to inertia inside the medium. In the figure below, change the tension and watch how far the wave travels in the same amount of time.
The conclusion of this first bonus installment. A wave is not something other than force; it's the "way force travels" when a restoring force and inertia are lined up across space. A single wiggle is carried from end to end by the chain of a force pulling the neighbor and inertia making it move a beat late. So asking "how fast is the wave?" is the same as asking "how are force and inertia balanced inside this medium?" The backbone of the main series, "force is a relationship," here takes the form of "a wave is the figure of force ── a relationship ── traveling through space."
Here we didn't write the wave equation itself; we described the "feel" of \(v=\sqrt{T/\mu}\) (the tug-of-war of restoring force ÷ inertia). Strictly, applying \(F=ma\) to the chain and taking the continuum limit gives the wave equation \(\partial^2 y/\partial t^2 = v^2\,\partial^2 y/\partial x^2\). Also, \(v=\sqrt{T/\mu}\) is for small displacements (the linear regime); for large amplitudes, or for media where the speed varies with wavelength (dispersion), it gets corrected.
The figure is a schematic of a transverse pulse; it is not a numerical solution of the actual motion of a spring chain (it only reproduces the point that the speed is proportional to √T).
Line a restoring force (the spring of Episode 3) and inertia (Episode 1) up across space, and a single wiggle propagates through the chain of "pull the neighbor → move a beat late → pull the next." That is a wave. A wave is not an independent entity; it's the figure of force and inertia traveling through space. Its speed is decided by a tug-of-war, \(v=\sqrt{T/\mu}=\sqrt{\text{restoring force}/\text{inertia}}\). A guitar string, sound, and even light can all be written with the same skeleton.
The main series' "force is a relationship" became, here, "a wave = the propagation of force, a relationship." Next time we go the other way ── the story that force itself was a wave. The field of the electromagnetic force is a nearby force when still, and a wave (light) that flies far away when you shake it. We'll see the two faces of one and the same field.
Print / PDF: ⌘+P (Ctrl+P on Windows). On screen, the slider lets you see the wave travel faster as you strengthen the tension. "See the answer" opens each solution.