The convolution theorem yields the given solution
x(t) = 1/2 ∫₀ᵗ f(t - τ) sin(2τ) dτ
How can you apply the convolution theorem to derive the indicated solution x(t)?²
Laplace transform of both sides of the equation: L{x''(t) + 4x(t)} = L{f(t)}
s² X(s) - sx(0) - x'(0) + 4X(s) = F(s)
Applying the convolution theorem to derive the indicated solution x(t)
x'(0) = 0: s² X(s) + 4X(s) = F(s)
X(s) = F(s) / (s² + 4)
Inversing Laplace transform
Recognize that X(s) is the product of F(s) and the Laplace transform of 1/2 sin(2t): X(s) = F(s) * (1/2) / (s² + 4)
Applying the convolution theorem
x(t) = 1/2 * L⁻¹ {F(s) * (1/2) / (s² + 4)} x(t) = 1/2 ∫₀ᵗ f(t - τ) sin(2τ) dτ
Therefore, the convolution theorem yields the given solution x(t):
x(t) = 1/2 ∫₀ᵗ f(t - τ) sin(2τ) dτ