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The inverse fourier transform of sgn(f)
  • a)
    -jπt
  • b)
    j/πt
  • c)
    1/jπt
  • d)
    None of these
Correct answer is option 'B'. Can you explain this answer?
Most Upvoted Answer
The inverse fourier transform of sgn(f)a)-jπtb)j/πtc)1/jπtd)N...

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The inverse fourier transform of sgn(f)a)-jπtb)j/πtc)1/jπtd)N...
The inverse Fourier transform of sgn(f)a)-j is given by:

F^(-1)[sgn(f)a)-j] = (1/2π) ∫[from -∞ to +∞] sgn(f)a)-j * e^(j2πft) df

To simplify this expression, we can consider the sign function sgn(f) separately. The sign function sgn(f) is defined as:

sgn(f) =
-1, if f < />
0, if f = 0,
1, if f > 0.

Since the sign function is only non-zero for positive values of f, the integral can be simplified to:

F^(-1)[sgn(f)a)-j] = (1/2π) ∫[from 0 to +∞] a)-j * e^(j2πft) df

Now, we can further simplify the expression by substituting a = |a|e^(jθ), where |a| is the magnitude of a and θ is the phase angle of a.

F^(-1)[sgn(f)a)-j] = (1/2π) ∫[from 0 to +∞] |a|e^(jθ) * e^(j2πft) df

Simplifying further, we get:

F^(-1)[sgn(f)a)-j] = (1/2π) |a| e^(jθ) ∫[from 0 to +∞] e^(j(2πf + θ)t) df

Using the property ∫[from -∞ to +∞] e^(jωt) dt = 2πδ(ω), where δ(ω) is the Dirac delta function, we can evaluate the integral:

F^(-1)[sgn(f)a)-j] = (1/2π) |a| e^(jθ) [2πδ(2πf + θ)]

Finally, simplifying the expression, we obtain:

F^(-1)[sgn(f)a)-j] = |a| e^(jθ) δ(2πf + θ)
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