Terminated String Impedance

Note that the impedance of the *terminated* string, seen from one
of its endpoints, is not the same thing as the wave impedance
of the string itself. If the string is infinitely
long, they are the same. However, when there are *reflections*,
they must be included in the impedance calculation, giving it an
imaginary part. We may say that the impedance has a ``reactive''
component. The driving-point impedance of a rigidly terminated string
is ``purely reactive,'' and may be called a *reactance* (§7.1).
If
denotes the force at the driving-point of the
string and
denotes its velocity, then the driving-point
impedance is given by (§7.1)

where and denote the Laplace transforms of and . In the case of a rigidly terminated string above, as well as in any system in which all energy delivered to the system is ultimately reflected back to the input, the impedance is purely imaginary at every frequency (a ``pure reactance''), as is easy to show:

where denotes the string length. Let denote the period of string vibration. Then on the frequency axis we have

Thus, the driving-point impedance of a rigidly terminated string is purely reactive (imaginary), with alternating poles and zeros along the axis. Impedance will be discussed further in §7.1 below.

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