Title | Fourier Transform Table |
---|---|
Author | Emma Cardenas |
Course | Linear Signals and Systems |
Institution | Johns Hopkins University |
Pages | 1 |
File Size | 59 KB |
File Type | |
Total Downloads | 66 |
Total Views | 148 |
Michael I. Miller...
2
Marc Ph. Stoecklin — TABLES OF COMMON TRANSFORM PAIRS — v1.6.1
Table of Continuous-time Frequency Fourier Transform Pairs f (t) = F −1 {F (f )} =
R +∞ −∞
F
F (f ) = F {f (t)} =
F (f )ej2πft df
⇐==⇒
f (t)
⇐==⇒
transform
F (f ) F (−f )
F
F ∗ (−f )
reversed conjugation
F
F ∗ (f )
complex conjugation
complex conjugation
f ∗ (t)
⇐==⇒
reversed conjugation
f ∗ (−t)
⇐==⇒
F (f ) = F ∗ (−f ) F (f ) = −F ∗ (−f )
f (t) = f ∗ (−t)
⇐==⇒
F
F (f ) is purely real
F
⇐==⇒
F (f ) is purely imaginary
F
F (f )e−j2πf t0
f (t − t0 )
⇐==⇒ ⇐==⇒
f (at) 1 f t |a| a
⇐==⇒
time scaling
linearity
F
⇐==⇒
F
F (f )G(f )
F
1
δ(t)
⇐==⇒
e−j2πft0 δ(f )
delta function
1
⇐==⇒
F
δ(f − f0 )
shifted delta function
a>0
⇐==⇒
F
ℜe{a} > 0
⇐==⇒
ℜe{a} > 0
F
⇐==⇒
2 e−πat
⇐==⇒
2a a2 +4π2 f 2 1 a+2πj f 1 a−2πj f πf 2 √1 e− a a
Gaussian function
Gaussian function
F
F
F
sine
sin (2πf0 t + φ)
⇐==⇒
cosine
cos (2πf0 t + φ)
⇐==⇒
sine modulation
f (t) sin (2πf0 t)
F
⇐==⇒
cosine modulation
f (t) cos (2πf0 t)
⇐==⇒
squared sine
sin2 (t)
⇐==⇒
squared cosine
cos2
triangular
triang
sinc
t T
=
T 1
= 0
1
−
|t| T
signum
sgn (t) =
1 (sgn(t) 2
n-th time derivative
⇐==⇒ ⇐==⇒
Dirac comb
P∞
n=0
F
F
⇐==⇒ F
sinc2π (B t)
F
1 −1
t>0 t0 t |t| 6 T |t| > T
0
squared sinc
constant
F
ej2πf0 t e−a|t|
t
frequency convolution frequency multiplication
⇐==⇒ F ⇐==⇒
constant
rect
frequency scaling
aF (f ) + bG(f )
⇐==⇒
δ(t − t0 )
rectangular
F (af )
F (f ) ∗ G(f )
f (t) ∗ g(t)
e−at u(t)
frequency shifting
F
⇐==⇒
e−at u(−t)
F (f − f0) f 1 F |a| a
F
⇐==⇒
shifted delta function
exponential decay
F
f (t)g (t)
delta function
two-sided exponential decay
F
af (t) + bg(t)
time multiplication time convolution
even/symmetry odd/antisymmetry
−f ∗ (−t)
f (t)ej2πf0 t
time shifting
reversed exponential decay
F
⇐==⇒ ⇐==⇒
f (t) =
frequency reversal
F
f (t) is purely real f (t) is purely imaginary odd/antisymmetry
f (t)e−j2πf t dt
F
⇐==⇒
even/symmetry
−∞
F
f (−t)
time reversal
R +∞
⇐==⇒ F
⇐==⇒ F
⇐==⇒
j 2 1 2 j 2 1 2 1 4 1 4
−j φ e δ (f + f0 ) − ej φ δ (f − f0 ) −j φ j φ e δ (f + f0 ) + e δ (f − f0 )
[F (f + f0 ) − F (f − f0 )]
[F (f + f0 ) + F (f − f0 )] 2δ(f ) − δ f − 1π − δ f + 1 2δ(f ) + δ f − π + δ f +
T sincπ (T f ) 2 (T f ) T sincπ f 1 rect B = |B| f 1 triang |B| B
⇐==⇒
1 1+t2
F ⇐= =⇒
δ(t − nf0 )
⇐==⇒
F
triangular
1 j πf
+ δ(f )
πe−2π|f | P∞ 1 f0
rectangular
signum
n (j2πf n) F (f ) j F (n) (f ) 2π n j δ (n) (f ) 2π
F
1 (f ) 1 ] ,+ B |B| [− B 2 2
sgn (f )
F
tn
squared sinc
inverse
1 2
⇐==⇒ F ⇐= =⇒
sinc
1 j πf
F
⇐==⇒
1 π 1 π
k=−∞
δ(f −
n-th frequency derivative
k f0
)...