Vector Formulation

Denote the sound-source velocity by $\underline{v}_s(t)$ where $t$ is time. Similarly, let $\underline{v}_l(t)$ denote the velocity of the listener, if any. The position of source and listener are denoted $\underline{x}_s(t)$ and $\underline{x}_l(t)$, respectively, where $\underline{x}\isdef (x_1,x_2,x_3)^T$ is 3D position. We have velocity related to position by

$$\underline{v}_s= \frac{d}{dt}\underline{x}_s(t) \qquad \underline{v}_l= \frac{d}{dt}\underline{x}_l(t). \protect$$ (4.7)

Consider a Fourier component of the source at frequency $\omega_s$. We wish to know how this frequency is shifted to $\omega_l$ at the listener due to the Doppler effect.

The Doppler effect depends only on velocity components along the line connecting the source and listener [327, p. 453]. We may therefore orthogonally project the source and listener velocities onto the vector $\underline{x}_{sl}=\underline{x}_l-\underline{x}_s$ pointing from the source to the listener. (See Fig. 3.16 for a specific example.)

The orthogonal projection of a vector $\underline{x}$ onto a vector ${\underline{y}}$ is given by [422]

$${\cal P}_{\underline{y}}(\underline{x}) = \frac{\left<\underline{... ...derline{x}^T{\underline{y}}}{{\underline{y}}^T{\underline{y}}}{\underline{y}}.$$

Therefore, we can write the projected source velocity as

$$\underline{v}_{sl}= {\cal P}_{\underline{x}_{sl}}(\underline{v}_s... ...line{x}_s\,\right\Vert^2}\left(\underline{x}_l-\underline{x}_s\right). \protect$$ (4.8)

In the far field (listener far away), Eq. (3.8) reduces to

$$\underline{v}_{sl} \approx \frac{\left<\underline{v}_s,\underline... ...derline{x}_l\,\right\Vert\gg\left\Vert\,\underline{x}_s\,\right\Vert). \protect$$ (4.9)