next previous
Up: Correction of the

Appendix A

Supposing a piston sequence of duration T. Let us define the standard deviation of piston during that sequence:
equation651
where tex2html_wrap_inline2368 is the average value of piston:
equation663
Let us consider the T-periodic function:
equation673
where tex2html_wrap_inline2372 and tex2html_wrap_inline2374 are, respectively, the window function of width T and the Dirac comb with spacing T. Then, tex2html_wrap_inline2380 equals tex2html_wrap_inline2382 on the interval tex2html_wrap_inline2384 and the moving average:
equation683
is a constant equal to tex2html_wrap_inline2386 by definition of tex2html_wrap_inline2388. Besides, the moving average acts as a low pass filter with transfer function tex2html_wrap_inline2390 on tex2html_wrap_inline2392. It is thus straightforward to derive the spectrum of the periodic function tex2html_wrap_inline2394 which matches tex2html_wrap_inline2396 on tex2html_wrap_inline2398:
equation700
with:
equation706
tex2html_wrap_inline2400 has discrete values with spacing tex2html_wrap_inline2402 and tex2html_wrap_inline2404. Hence, for tex2html_wrap_inline2406:
equation717
and the spectrum is zero except for harmonics:
equation729
Computing the standard deviation for a piston sequence of duration T thus amounts to computing the standard deviation of the periodic function tex2html_wrap_inline2410 which is the square root of the infinite sum of the squared harmonics. Eventually:
equation739


Copyright by the European Southern Observatory (ESO)
web@ed-phys.fr