F ( f ( x ) ) = 2 π ∫ 0 ∞ f ( x ) sin ( ω x ) d x F ( 1 ) = 2 π ∫ 0 l 1 × sin ( ω x ) d x = 2 π ∫ 0 l sin ( ω x ) d x = 2 π ∫ 0 l − cos ( ω x ) ω d x = 2 π ⋅ − cos ( ω x ) ω ∣ 0 l = 2 π ⋅ cos ( ω x ) ω ∣ l 0 = 2 π ( 1 − cos ( l ω ) ω ) \displaystyle
\mathcal{F}(f(x)) = \sqrt{\frac{2}{\pi}}\int_0^\infty f(x)\sin(\omega x) \, \mathrm{d}x\\
\begin{aligned}
\mathcal{F}(1) &= \sqrt{\frac{2}{\pi}}\int_0^l 1 \times \sin(\omega x) \, \mathrm{d}x = \sqrt{\frac{2}{\pi}}\int_0^l \sin(\omega x) \, \mathrm{d}x
\\&= \sqrt{\frac{2}{\pi}}\int_0^l \frac{-\cos(\omega x)}{\omega} \, \mathrm{d}x
\\&= \sqrt{\frac{2}{\pi}}\cdot \frac{-\cos(\omega x)}{\omega}\biggr\vert_0^l = \sqrt{\frac{2}{\pi}} \cdot \frac{\cos(\omega x)}{\omega}\biggr\vert_l^0
\\&= \sqrt{\frac{2}{\pi}}\left(\frac{1 - \cos(l\omega)}{\omega}\right)
\end{aligned} F ( f ( x )) = π 2 ∫ 0 ∞ f ( x ) sin ( ω x ) d x F ( 1 ) = π 2 ∫ 0 l 1 × sin ( ω x ) d x = π 2 ∫ 0 l sin ( ω x ) d x = π 2 ∫ 0 l ω − cos ( ω x ) d x = π 2 ⋅ ω − cos ( ω x ) ∣ ∣ 0 l = π 2 ⋅ ω cos ( ω x ) ∣ ∣ l 0 = π 2 ( ω 1 − cos ( l ω ) )