Superposition and Reflection

When multiple waves occupy the same place, the medium does not choose one wave and ignore the others. The visible disturbance is the superposition of all individual waves:

total wave=wave 1+wave 2+\text{total wave} = \text{wave 1} + \text{wave 2} + \cdots

That means wave amplitudes add point by point, and two waves can amplify or cancel one another locally.

left componentright componenttotal

Separate pulses: the total wave mostly matches each individual pulse.

Boundaries as Constraints

Now consider waves near a boundary. An incident wave is the wave arriving at the boundary. A reflected wave is the part sent back into the original medium. A transmitted wave is the part that continues into the next medium, if the next medium can respond.

Although the particular physics that cause reflection and transmission (i.e. medium-dependent forces) may differ, it is convenient to reason about the so-called boundary conditions. These are local demands placed on the total wave. For example, the displacement must be zero at a fixed end of string. The reflected wave therefore comes back inverted so the incident and reflected displacements cancel exactly at this fixed end.

Air Boundaries

Like strings, air-filled tubes (flutes, PVC pipes, pipe organs etc.) support similar wave phenomena. A full description of what individual air molecules are actually doing is rather complex, but there are two macroscopic quantities that are convenient to describe:

  • Pressure tells us how compressed (more dense) or rarefied (less dense) the air is.
  • Displacement tells us how the air, when treated as a fluid, is moving back and forth.

The two descriptions are related, but they do not peak in the same place. Pressure is about crowding: if neighboring regions of air move toward each other, the air between them compresses; if they move apart, it rarefies. Displacement is about how regions of air have shifted from equilibrium. In a traveling sound pulse, the crowding shows up slightly ahead of the largest displacement.

When starting, pick whichever is more intuitive; in the long run both descriptions give equivalent results. For example, a closed pipe wall stops the air motion. This means a closed end is a displacement node and a pressure antinode. An open pipe end does almost the opposite: the pressure variation near the opening stays close to the outside atmospheric pressure, so the open end is a pressure node and a displacement antinode.

It is tempting to think an open end should simply let the wave leave. Some energy really does radiate outward as sound. But an open end is still a sharp change from a narrow guided air column to a large outside space.

Sound boundary

Open pipe end

incoming mediumoutside airboundary: pressure nodePressure variationpressure nodeAir displacementdisplacement antinodeincident pulsereflected pulsetransmitted pulsetotal

Open does not mean boundary-free. The pressure variation at the opening stays near atmospheric pressure, so a reflected pressure wave cancels the incident pressure while some sound radiates outward.

From Reflections to Standing Waves

When a source keeps driving the same system, the incident and reflected waves overlap again and again. Most driving frequencies result in a mess of partial reinforcement and cancellation. Special frequencies make the phase line up so the total pattern repeats in place. Those are the standing waves and harmonics on the next page.

Problem Solving

Fixed-End Reflection

Problem

A string pulse reaches a fixed end. At the boundary, the incident displacement would be +2 cm+2\ \text{cm}. What reflected displacement is needed at that instant?

Solve

A fixed end must stay at zero total displacement:

yincident+yreflected=0.y_{\text{incident}} + y_{\text{reflected}} = 0.

So the reflected displacement must be 2 cm-2\ \text{cm}, which is the inverted pulse value.

Open and Closed Pipe Ends

Problem

Classify the displacement and pressure behavior at the ends of an ideal pipe: one end closed, one end open.

Reasoning

At a closed end, the air cannot move through the wall, so displacement is a node and pressure is an antinode. At an open end, pressure stays near the outside atmospheric pressure, so pressure is a node and displacement is an antinode.

Reflection Checkpoint

Question 1 of 3

Why can a sound wave reflect from the open end of a pipe?

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