In order to carry out frequency-domain synthesis of plucked strings as described in section 5.4, we need two frequency response functions related to the string: the drive-point admittance (or in fact its inverse, the *impedance*) at the end of the string, and also the transfer function linking motion at the end to motion at the required plucking point.

These need to incorporate the effects of bending stiffness and damping, derived in sections 5.4.4 and 5.4.5. The same trick can be used for both functions. We first solve the problem for the ideal string without damping or stiffness: there are analytic formulae for both functions. We then expand the resulting expressions in partial fractions, interpret the terms as corresponding to the modes of the string, then adjust the complex pole frequencies to allow for stiffness and damping, without changing anything else.

Suppose the string is fixed at position $x=0$, and that a harmonic displacement $y e^{i \omega t}$ is imposed at $x=L$. To satisfy the fixed boundary condition, the string displacement must take the form

$$w=k \sin \frac{\omega x}{c} \tag{1}$$

where $k$ is a constant, and $c=\sqrt{P/m}$ is the wave speed on the string. Imposing the other boundary condition fixes the value of $k$, so that

$$w=y \dfrac{ \sin (\omega x/c)}{ \sin (\omega L/c)} \tag{2}$$

This gives the first of our two frequency response functions, $w/y$.

Now if the end motion is caused by a force $f e^{i \omega t}$ applied to the string, force balance requires

$$f=P \left. \dfrac{\partial w}{\partial x} \right|_{x=L}=\dfrac{Py\omega \cos(\omega L/c)}{c \sin (\omega L/c)} \tag{3}$$

so the required end impedance is

$$Z(\omega)=\frac{f}{i \omega y}=\frac{P}{ic} \cot \frac{\omega L}{c}=-i Z_{string} \cot \frac{\omega L}{c} \tag{4}$$

in terms of the string’s characteristic impedance $Z_{string}=\sqrt{Pm}$.

The impedance $Z$ has *poles* (resonances) where

$$\frac{\omega L}{c} = n \pi, \mathrm{~~~for~~~}n=0, \pm 1,\pm 2,\pm 3… \tag{5}$$

The function is obviously periodic, so that the coefficients, called *residues*, of these poles must all have the same value. This value can be found by looking at the behaviour near $\omega=0$, where

$$\frac{P}{ic}\cot \frac{\omega L}{c} \approx \frac{P}{ic} \times \frac{c}{\omega L}=\frac{-iP}{\omega L}. \tag{6}$$

We can deduce that

$$Z(\omega) = -\frac{iP}{L} \sum_{n=-\infty}^{\infty}{\dfrac{1}{\omega – n \pi c/L}} . \tag{7}$$

We can add small damping with loss factor $\eta_j$ for the $j$th mode, and regroup the terms to look more like the familiar modal summation:

$$Z(\omega) = -\frac{iP}{L} \left[ \frac{1}{\omega} + \sum_{j=0}^{\infty}{\left\lbrace \dfrac{1}{\omega – \omega_j(1+i \eta_j /2)}+\dfrac{1}{\omega + \omega_j(1-i \eta_j /2)}\right\rbrace} \right] $$

$$=-\frac{iP}{L} \left[ \frac{1}{\omega} + \sum_{j=1}^{\infty}{ \dfrac{2 \omega – i \omega_j \eta_j}{\omega^2 – i\omega \omega_j \eta_j – \omega_j^2}} \right] \tag{8}$$

where we can now substitute for $\omega_j$ the approximate formula including the effect of bending stiffness, from eq. (10) of section 5.4.3.

A similar procedure can be applied to the other frequency response function of interest, $w/y$ from eq. (2), to provide an approximation to the transfer function from the end of the string to the plucking point $x=a$, including the effects of damping and bending stiffness. The result is

$$\frac{w}{y} \approx \frac{a}{L} + \frac{c}{L}\sum_{j=1}^{\infty}{ (-1)^j \dfrac{2 \omega \sin j \pi a/L}{\omega^2 – i\omega \omega_j \eta_j – \omega_j^2}} . \tag{9}$$