Dashboard/Learning Hub/Physics HL/Chapter 14/14.2 The Principle of Superposition

Physics HL · Chapter 14: Wave Phenomena

14.2 The Principle of Superposition

Use algebraic displacement addition to analyze pulse overlap, constructive and destructive interaction, and boundary reflection phase changes.

Estimated time: 30 minutes

Superposition as a Local Rule

y(x,t)=y1(x,t)+y2(x,t)+y(x,t) = y_1(x,t) + y_2(x,t) + \cdots

At each location and time, the medium displacement equals the algebraic sum of contributions from all waves present.

Superposition is local in space and time. You do not add wave amplitudes globally once; you add displacements point-by-point while overlap exists. After overlap, each pulse continues with its original shape and speed in ideal linear media. This is the core contrast with colliding particles, which exchange momentum and do not pass through each other unchanged.

The word algebraic is essential. Opposite signs can cancel and same signs can reinforce. If two equal pulses with opposite displacements perfectly overlap, instantaneous displacement can be zero everywhere, but that does not mean energy disappears permanently. It is redistributed in the oscillatory field and pulse evolution.

Constructive and Destructive Overlap

Constructive overlap occurs when displacements share sign at a point, increasing magnitude. Destructive overlap occurs when signs oppose, reducing magnitude. Most exam sketches ask for an intermediate overlap shape, so the fastest workflow is to draw each pulse lightly and sum their heights at several reference points.

Linear superposition also underpins interference patterns later in this chapter. Two-slit bright and dark fringes are not a separate principle; they are repeated superposition outcomes across many observation points with systematically varying phase difference.

Reflection of Pulses at Fixed and Free Ends

At a fixed end, boundary displacement must remain zero, so the reflected pulse inverts (180 degree phase shift). At a free end, boundary force condition differs and reflection can occur without inversion. These boundary phase rules become important in standing-wave formation in the next chapter.

A useful mental model is to enforce the boundary condition first, then infer reflected sign. If the endpoint cannot move, the reflected contribution must cancel incident displacement at that point. If the endpoint can move freely, cancellation is not required in the same way.

Simulation: Pulse Superposition Timeline

Adjust pulse amplitudes, widths, and velocities to inspect constructive and destructive overlap and post-overlap recovery.

Wave Phenomena Studio

Current mode: Pulse Superposition

Pulse 1Pulse 2Sum y = y1 + y2

Pulse 1 center

1.20 m

Pulse 2 center

-1.20 m

Overlap index

0.00e+0 %

The pulses pass through each other while the instantaneous displacement at each point is the algebraic sum of the two contributions. Try opposite-sign amplitudes for destructive interference and same-sign amplitudes for constructive overlap.

Test Yourself

Two pulses start 0.80 m apart and move toward each other at 2.0 m/s and 3.0 m/s. Enter the time to complete overlap of their centers.

Hint: Use relative speed for approach motion.