- 2069 Chaitra · 5 marks
Second shifting theorem
Short answer
If L[f(t)]=F(s) then L[f(t-a)u(t-a)]=e^(-as)F(s). Proof: L[f(t-a)u(t-a)] = ∫_a^∞ e^(-st)f(t-a)dt, substitute τ=t-a → e^(-as)∫_0^∞ e^(-sτ)f(τ)dτ = e^(-as)F(s).
State and prove the second shifting theorem of the Laplace transform.
Statement
If L[f(t)] = F(s) and
g(t) = f(t − a) for t > a
g(t) = 0 for t < a (a > 0)
i.e. g(t) = f(t − a) u(t − a) with u the unit step function, then
L[g(t)] = e^(−as) F(s)
Equivalently, L⁻¹[e^(−as) F(s)] = f(t − a) u(t − a).
Proof
L[g(t)] = ∫₀^∞ e^(−st) g(t) dt
= ∫₀^a e^(−st)·0 dt + ∫ₐ^∞ e^(−st) f(t − a) dt
In the second integral put τ = t − a. Then t = τ + a, dt = dτ, and the limits become τ = 0 to ∞:
L[g(t)] = ∫₀^∞ e^(−s(τ + a)) f(τ) dτ
= e^(−as) ∫₀^∞ e^(−sτ) f(τ) dτ
= e^(−as) F(s)
∎
Example
L[u(t − 2)(t − 2)] = e^(−2s)/s². Also, L[u(t − a)] = e^(−as)/s (take f(t) = 1).
✓ Answer checked by Claude Opus 5.5 (high effort)
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