Laplaceovo desatero Fourierovo desatero L[f(ct)] = 1cF(pc) F[f(c⃗x)] = |c1|rF(ξ⃗c) L[(−t)nf(t)] =ddpnFn F[(i⃗x)αf(⃗x)] =DαF[f(⃗x)]
L[ ˙f(t)] =pL[f(t)]−f(0+) F[Dα( f(⃗x))
] = (−i⃗ξ)αF[f(⃗x)]
L[Θ(t)∫t
0 f(τ)dτ] = F(p)p F[1] = (2π)rδ(⃗ξ) L[f(t)t ] =∫∞
p F(q)dq FF[f(x)] = (2π)rf(−x) eapL[f(t)] =L[f(t+a)] ei⃗µ⃗ξF[f(⃗x)] =F[f(⃗x−⃗µ)]
L[eatf(t)] =F(p−a) F[ei⃗µ⃗xf(⃗x)] =F(⃗ξ+⃗µ)
∫∞
0 f(τ)dτ = limp→0+F(p) lim|ξ|→∞F(ξ) = 0 L[f(t) ⋆ g(t)] =F(p)·G(p) F[f(⃗x)⋆ g(⃗x)] =F[f(⃗x)]·F[g(⃗x)]
∫∞
0 f(t)G(t)dt=∫∞
0 F(t)g(t)dt ∫∞
−∞f(x)G(x)dx=∫∞
−∞F(x)g(x)dx
Laplace·v vzor Laplace·v obraz δ(t−τ) e−pτ
Θ(t) 1p
Θ(t)tn (n∈N0) pn+1n!
Θ(t)tα (α >−1) Γ(α+1)pα+1
Θ(t)eµt p−1µ
Θ(t) sin(βt) p2+ββ 2
Θ(t) cos(βt) p2+βp 2
Θ(t) (sin(t)−tcos(t)) (1+p22)2
Θ(t)eµtcos(ωt) (p−pµ)−2µ+ω2
Θ(t)eµtsin(ωt) (p−µ)ω2+ω2 Θ(t) sinh(ωt) p2−ωω2 Θ(t) cosh(ωt) p2−pω2
Fourie·v vzor Fourie·v obraz Obor e−a∥x∥2 (πa)r/2e−∥
⃗ξ∥2
4a Er
Θ(x)eax, (a̸= 0) a+iξ−1 R
δ(⃗x−⃗µ) ei⃗ξ⃗µ Er
Θ(x) πδ(ξ) + iP1ξ R
Θ(−x) πδ(ξ) −iP1ξ R
sgn(x) 2iP1ξ R
1 (2π)rδ(⃗ξ) Er
Px1 iπsgn(ξ) R
Px12 −π|ξ| R
eix2 √
πe−4i(ξ2−π) R
Θ(R− |x|) 2sin(Rξ)ξ R
Θ(R−∥⃗x∥)
√R2−∥⃗x∥2 2πsin(R∥⃗ξ∥)
∥⃗ξ∥ E2 δSR(⃗x) 4πRsin(R∥⃗ξ∥)
∥⃗ξ∥ E3
⃗
xα (i)|α|(2π)rδ(α)(ξ)⃗ Er
eicx 2πδ(ξ+c) R
cos(cx) π(
δ(ξ−c) +δ(ξ+c)) R
sin(cx) iπ(
δ(ξ−c)−δ(ξ+c)) R