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Physics · Ch 6 — Superposition of Waves

Reflection of a Transverse Wave

6.3.1

Reflection of a Transverse Wave

Consider a long, light string with one end (B) attached to a perfectly rigid support, representing the boundary between a rarer medium (the light string itself) and a denser medium (the immovable support). Giving the free end (A) a jerk sends a single crest travelling towards B. As the crest reaches B, it tries to pull point B upward -- but B, being rigidly fixed, cannot move; by Newton's third law, an equal and opposite reaction then acts back on the string, pulling it DOWNWARD instead. The observed result is that the crest returns from the fixed end as a TROUGH: reflection at a rigid support (a denser medium) inverts the wave. Since a crest and a trough of the same wave differ in phase by exactly π\pi radians, we say reflection from a fixed end (denser medium) introduces a phase change of π\pi radians.

Now suppose instead the string's end B is attached to a light ring that can slide freely, without friction, along a vertical rod -- this end is effectively free to move, representing a boundary with a RARER medium. When the crest reaches the ring, it genuinely pulls the ring upward with it, and the pulse is observed to reflect back still as a CREST, with no inversion -- reflection from a free (rarer-medium) end introduces NO phase change. …

Figure 6.1Reflection of a transverse wave pulse sent as a crest from a rarer medium to a denser medium — the crest reflects as a trough (phase change of π)
Fig. 6.1 — Reflection of a transverse wave pulse sent as a crest from a rarer medium to a denser medium — the crest reflects as a trough (phase change of π)

Drawn by us to help you understand the concept clearly, and verified to make sure it's accurate. For exams, practice from your textbook's own diagram.

What this figure shows. A crest travelling along a light string AB toward a rigid support at B (the string is the rarer medium, the rigid support the denser medium). On reaching the fixed end the crest is reflected back as a TROUGH — an inversion — because the rigid support cannot move and, by Newton's third law, pulls the string the opposite way. So reflection from a …

Figure 6.2Reflection of a transverse wave pulse sent as a crest from a denser medium to a rarer medium — the crest reflects as a crest (no phase change)
Fig. 6.2 — Reflection of a transverse wave pulse sent as a crest from a denser medium to a rarer medium — the crest reflects as a crest (no phase change)

Drawn by us to help you understand the concept clearly, and verified to make sure it's accurate. For exams, practice from your textbook's own diagram.

What this figure shows. A crest travelling along a string whose end B is attached to a light ring that slides freely on a frictionless rod (the free end behaves as a rarer medium). On reaching the free end the crest is reflected back as a CREST — no inversion — because the ring is free to move up. So reflection f …

Figure 6.3Reflection of a crest at the junction of a heavy string and a light string — (a) from the denser (heavy) string the crest reflects as a trough, (b) from the rarer (light) string it reflects as a crest
Fig. 6.3 — Reflection of a crest at the junction of a heavy string and a light string — (a) from the denser (heavy) string the crest reflects as a trough, (b) from the rarer (light) string it reflects as a crest

Drawn by us to help you understand the concept clearly, and verified to make sure it's accurate. For exams, practice from your textbook's own diagram.

What this figure shows. A heavy string P and a light string Q are joined at O. (a) A crest travelling on the heavy string (denser medium) toward O is reflected as a trough — an inversion, phase change π. (b) A crest travelling on the light string (rarer medium) toward O is reflected as a crest — no inversion, no phase change. The reflecte …