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Why substitute t=0t = 0 into the inverse Fourier transform to evaluate the Dirichlet integral?

Substituting t=0t = 0 into the inverse Fourier transform formula simplifies the exponential term eiωte^{i\omega t} to 1, removing the oscillatory component from the integrand. This transforms the inverse transform equation into a direct relationship between the value of the original function at the origin, f(0)f(0), and the integral of its Fourier transform F(ω)F(\omega) over the entire real line. Since f(0)=1f(0) = 1 for the rectangular pulse and F(ω)=2sin⁡ωωF(\omega) = 2 \frac{\sin \omega}{\omega}, this substitution allows us to set up the equation 1=12π∫−∞∞2sin⁡ωωdω1 = \frac{1}{2\pi} \int_{-\infty}^{\infty} 2 \frac{\sin \omega}{\omega} d\omega, which can be algebraically manipulated to isolate the Dirichlet integral ∫0∞sin⁡ωωdω\int_{0}^{\infty} \frac{\sin \omega}{\omega} d\omega.

Conditions

  • The inverse Fourier transform formula is f(t)=12π∫−∞∞F(ω)eiωtdωf(t) = \frac{1}{2\pi} \int_{-\infty}^{\infty} F(\omega) e^{i\omega t} d\omega.
  • The function f(t)f(t) is the rectangular pulse with f(0)=1f(0)=1.
  • F(ω)F(\omega) is the previously computed Fourier transform 2sin⁡ωω2 \frac{\sin \omega}{\omega}.

Reasoning, step by step

  1. Recall the inverse Fourier transform formula: f(t)=12π∫−∞∞F(ω)eiωtdωf(t) = \frac{1}{2\pi} \int_{-\infty}^{\infty} F(\omega) e^{i\omega t} d\omega.
  2. Choose t=0t = 0 to eliminate the complex exponential term: eiω⋅0=e0=1e^{i\omega \cdot 0} = e^0 = 1.
  3. Evaluate the left-hand side using the definition of the rectangular pulse: f(0)=1f(0) = 1.
  4. Substitute the known expression for F(ω)F(\omega) on the right-hand side: F(ω)=2sin⁡ωωF(\omega) = 2 \frac{\sin \omega}{\omega}.
  5. Set up the equation: 1=12π∫−∞∞2sin⁡ωωdω1 = \frac{1}{2\pi} \int_{-\infty}^{\infty} 2 \frac{\sin \omega}{\omega} d\omega.
  6. Simplify the constants: 1=1π∫−∞∞sin⁡ωωdω1 = \frac{1}{\pi} \int_{-\infty}^{\infty} \frac{\sin \omega}{\omega} d\omega.
  7. Rearrange to solve for the full-axis integral: ∫−∞∞sin⁡ωωdω=π\int_{-\infty}^{\infty} \frac{\sin \omega}{\omega} d\omega = \pi.
  8. Use the evenness of sin⁡ωω\frac{\sin \omega}{\omega} to find the half-axis integral: ∫0∞sin⁡ωωdω=π2\int_{0}^{\infty} \frac{\sin \omega}{\omega} d\omega = \frac{\pi}{2}.
  9. Conclude that substituting t=0t=0 is the key step that links the specific function value to the desired improper integral.

Example

The video states: 'The instructor chose to set t=0t = 0 on both sides of the equation. At this point, the original function satisfies f(0)=1f(0) = 1, and the exponential term becomes eiω⋅0=1e^{i\omega \cdot 0} = 1. Thus, the inverse transform formula reduces to 1=12π∫−∞∞F(ω)dω1 = \frac{1}{2\pi} \int_{-\infty}^{\infty} F(\omega) d\omega'.

Common misconceptions

  • Thinking that t=0t=0 is arbitrary; it is chosen specifically because f(0)f(0) is known and non-zero, and it simplifies the kernel to 1.
  • Assuming the integral converges absolutely at t=0t=0 without considering the principal value or the specific properties of the sinc function; the video treats it as a standard improper integral evaluation.
  • Confusing the forward and inverse transform formulas; the substitution is made in the inverse formula.

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