time average of harmonic power. Expand the two real parts:
The terms proportional to average to zero over complete periods, while is time-independent. For real peak amplitudes this is .
String dynamics. A short element of length experiences transverse force . Newton's second law therefore gives , or
The approximation is a flexible, lossless string with small slope and constant tension; is its linear mass density.
energy transport. Across a cut toward increasing , the transverse force is and the transverse velocity is . For a rightgoing wave these have complex amplitudes and . Hence
This real mechanical impedance is force divided by transverse velocity for a travelling wave, with units .
Matching and power ratios. At an ordinary massless junction without an external transverse force, displacement is continuous and transverse tension is balanced: , . For the same tension, the slope is therefore continuous even if density changes. With real positive impedances,
Their sum equals ; the transmitted power includes the impedance ratio and is not simply .
Substituting into the junction formula gives
Equal densities give zero reflection; a very large mismatch gives nearly complete reflection. reflection from the higher-impedance side reverses displacement phase.
At the zero-slope boundary, the rightgoing and leftgoing slopes cancel, so . Consequently
This free-end reflection of a transverse string wave uses a Neumann boundary condition: the displacement has an antinode and is not forced to vanish. The instantaneous flux through the boundary is zero, confirming that it transmits no power.

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