P. 542, last boxed set of equations

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The first equation should be

a_{m,n} = \frac{\hat r}{\alpha z_{m,n}} \frac{\int_0^{\hat r} \int_0 ^{2 \pi} r f(r, \theta) \cos m \theta J_m (z_{m,n} r/\hat r) d \theta dr}{\left( \int_0^{2 \pi} \cos^2 m \theta d \theta \right) \left(\int_0^{\hat r} r J^2_m (z_{m,n} r/\hat r) \right)}</math>

The second equation should be

b_{m,n} = \frac{\hat r}{\alpha z_{m,n}} \frac{\int_0^{\hat r} \int_0 ^{2 \pi} r f(r, \theta) \sin m \theta J_m (z_{m,n} r/\hat r) d \theta dr}{\left( \int_0^{2 \pi} \cos^2 m \theta d \theta \right) \left(\int_0^{\hat r} r J^2_m (z_{m,n} r/\hat r) \right)}</math>

The third equation should be

cm,n=r^αzm,n0r^02πrg(r,θ)cosmθJm(zm,nr/r^)dθdr(02πcos2mθdθ)(0r^rJm2(zm,nr/r^))

and the fourth equation should be

dm,n=r^αzm,n0r^02πrg(r,θ)sinmθJm(zm,nr/r^)dθdr(02πcos2mθdθ)(0r^rJm2(zm,nr/r^)).


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