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The propogating wavefront generates spherical wavelets as it propogates. What we want to know is what the wave at the initial point <math> f(x,y,0,t) </math> will look like at <math>f(x,y,D,t)</math>. To do this, we can integrate over the product of this equation times a propogator g.
The propogating wavefront generates spherical wavelets as it propogates. What we want to know is what the wave at the initial point <math> f(x,y,0,t) </math> will look like at <math>f(x,y,D,t)</math>. To do this, we can integrate over the product of this equation times a propogator g.
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<math> g( x_i, t_i, x_f, t_f)
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<math> g( x_i, t_i, x_f, t_f)\,</math>
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Because the propogator is actually in terms
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Because the propogator is actually in terms of the differences between the x and t values, we will write the difference between the x-vectors as <math>\Delta x</math> and the difference between the times as <math>\Delta t</math>.
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of the differences between these values, we will
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write the difference between the x-vectors as
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{delta, hereafter d} dx and the difference between
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the times as dt.
[integral]dti [integral]g(stuff)f(stuffi)dxi dyi =
[integral]dti [integral]g(stuff)f(stuffi)dxi dyi =