Reflectance of the Conical Cap

Let ${t_{\xi}}\isdef \xi/c$ denote the time to propagate across the length of the cone in one direction. As is well known [22], the reflectance at the tip of an infinite cone is $-1$ for pressure waves. I.e., it reflects like an open-ended cylinder. We ignore any absorption losses propagating in the cone, so that the transfer function from the entrance of the cone to the tip is $e^{-s{t_{\xi}}}$ . Similarly, the transfer function from the conical tip back to the entrance is also $e^{-s{t_{\xi}}}$ . The complete reflection transfer function from the entrance to the tip and back is then

$$R_{t_{\xi}}(s) = - e^{-2s{t_{\xi}}}$$ (C.152)

Note that this is the reflectance a distance $\xi=c{t_{\xi}}$ from a conical tip inside the cone.

We now want to interface the conical cap reflectance $R_{t_{\xi}}(s)$ to the cylinder. Since this entails a change in taper angle, there will be reflection and transmission filtering at the cylinder-cone junction given by Eq.(C.151) and Eq.(C.152).

From inside the cylinder, immediately next to the cylinder-cone junction shown in Fig.C.48, the reflectance of the conical cap is readily derived from Fig.C.48b and Equations (C.151) and (C.152) to be

$$R_J(s) = \frac{R(s) + 2 R(s) R_{t_{\xi}}(s) + R_{t_{\xi}}(s)}{1 - R(s)R_{t_{\xi}}(s)} = \frac{1 + (1+2s{t_{\xi}})R_{t_{\xi}}(s)}{2s{t_{\xi}}-1-R_{t_{\xi}}(s)}$$

$$= \frac{1 - (1+2s{t_{\xi}})e^{-2s{t_{\xi}}}}{2s{t_{\xi}}-1+e^{-2s{t_{\xi}}}} \isdef \frac{N(s)}{D(s)}$$ (C.153)

where

$$N(s) \isdef 1 - e^{-2s{t_{\xi}}} - 2s{t_{\xi}}e^{-2s{t_{\xi}}}$$ (C.154)

is the numerator of the conical cap reflectance, and

$$D(s) \isdef 2 s{t_{\xi}}- 1 + e^{-2s{t_{\xi}}}$$ (C.155)

is the denominator. Note that for very large ${t_{\xi}}$ , the conical cap reflectance approaches $R_J = -e^{-2s{t_{\xi}}}$ which coincides with the impedance of a length $\xi=c{t_{\xi}}$ open-end cylinder, as expected.