To obtain this, set
; apply the Fourier transform to the normalwash at midchord:
.
To use this, we must first develop an expression for cl for a case of simple harmonic gust velocity variation, then substitute the indicial gust expression n the frequency domain. As before, we seek a generalized expression where the complicated parts of the integral are computed as a general function.
Simple harmonic transverse gust:
In flow-fixed coordinates,
, a simple harmonic spatial function. In terms of
, non-dimensional body-fixed coordinates,
; periodic in space and time.
Substitute in our expression for Cp in the frequency domain. Now
and
. Substituting for Cp, we get (skipping some math here),
, and
.
Define
. Thus
.
Transform cl(k,t) into the frequency domain:
and
and
. Substituting for
, with
(semi-chords traveled in time t),
;
.
is the Kussner Function.