The symbol here is linear mass density, with units . A short element has transverse forcebecause small slopes give . Its mass is . Applying Newton's second law, dividing by , and taking the limit gives the wave equation on a string,The derivation assumes constant positive tension, small transverse displacements and slopes, a flexible string with negligible bending stiffness, and negligible damping. Variations of tension due to the motion enter beyond the linear approximation.
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