Consider a periodic signal π T = 2g(t) = ∑_k=-[infinity][infinity] δ (t-2k)T = 2(dx(t))(dt) = A₁ g(t-t₁) + A₂ g(t-t₂) π. π A₁ π, π t₁ π, π A₂ π π t₂ π
a) π T = 2 π
b) π g(t) = ∑_k=-[infinity][infinity] δ (t-2k) π
c) π A₁, t₁, A₂, t₂ π
d) π dx(t)dt π