Let the uniform string have constant tension and linear mass density . Assume small transverse motion with , negligible longitudinal motion, and no external transverse force. If the string makes angle with the horizontal, then , and the small-angle approximation gives and to first order.
The net upward force on the segment from to is therefore
By Newton's second law, its mass times its transverse acceleration equals this force, to the order retained in the small displacement model. Divide by and let to obtain
Thus the wave equation on a string is
where is the wave speed. The horizontal force balance makes the horizontal component of tension constant; to first order it equals .

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