awelex
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Hi,
I'm trying to adapt the doppler shift formula for a stationary listener and a source traveling in a straight line towards/away from the listener to the case where the source does not move straight towards the listener. For example, suppose that I am looking north and train further in the distance moves from west to east.
The frequency factor in the 1D case is \frac{v}{v - 333m/s}. The only thing that changes in the 2D case is that we can't no longer use the absolute velocity v of the source, but have to use the relative velocity with respect to the listener. But this is where I'm stuck: How do I compute this relative velocity when the listener is stationary? Wouldn't that mean that v_{rel} = v_{abs} - 0 = v_{abs}? That obviously can't be true.
Thanks,
Alex
I'm trying to adapt the doppler shift formula for a stationary listener and a source traveling in a straight line towards/away from the listener to the case where the source does not move straight towards the listener. For example, suppose that I am looking north and train further in the distance moves from west to east.
The frequency factor in the 1D case is \frac{v}{v - 333m/s}. The only thing that changes in the 2D case is that we can't no longer use the absolute velocity v of the source, but have to use the relative velocity with respect to the listener. But this is where I'm stuck: How do I compute this relative velocity when the listener is stationary? Wouldn't that mean that v_{rel} = v_{abs} - 0 = v_{abs}? That obviously can't be true.
Thanks,
Alex