Open abhayku2002 opened 9 months ago
from sympy import * from sympy.plotting import plot from sympy.abc import x, k,t,f,i,j
func2 = exp(2piift) inverse_fourier_transform(func2, f, t)
`from sympy import * from sympy.plotting import plot from sympy.abc import x, k,t,f,i,j
func2 = exp(2piift) inverse_fourier_transform(func2, f, t)`
from sympy.plotting import plot
from sympy.abc import x, k,t,f,i,j
func2 = exp(2*pi*i*f*t)
inverse_fourier_transform(func2, f, t)```
from sympy.plotting import plot
from sympy.abc import x, k,t,f,i,j
func2 = exp(2*pi*i*f*t)
inverse_fourier_transform(func2, f, t)
from sympy.plotting import plot
from sympy.abc import x, k,t,f,i,j
func2 = exp(2*pi*i*f*t)
inverse_fourier_transform(func2, f, t)
\displaystyle e^{- 2 i \pi t}
`\displaystyle e^{- 2 i \pi t}
`
\displaystyle e^{- 2 i \pi t}
$\displaystyle e^{- 2 i \pi t}
$
In the Inverse Fourier Transform, omega
and t
represent the frequency and time variables
from sympy import *
from sympy.plotting import plot
from sympy.abc import x, k,t,omega,i,j
delta = DiracDelta(omega - 1)
inverse_fourier_transform(delta, omega, t)
Output:
$\displaystyle e^{2 i \pi t}
$
here is the `from sympy import * from sympy.plotting import plot from sympy.abc import x, k,t,f,i,j
func2 = exp(2piift) inverse_fourier_transform(func2, f, t)`