1b
0.693b
2b
b
Consider the free body diagram shown in the figure. For the equilibrium in the normal direction, we have T=mgcosθ In the tangential direction, mLθ'' = -mgsinθ -mbv For small angle θ, we have sinθ ≈ θ and v=Lθ̇ Thus, mLθ'' + mbLθ̇ + mgθ = 0 Solution to the above differential equation is θ(t) = θ0e^(-bt/2)sin(ωdt+φ) Let average lifetime be τ. Amplitude at t=0 is θ0 and amplitude at t=τ is θ0e^(-bτ/2) But the ratio is equal to 1/e Thus, e^(-bτ/2) = e⁻¹ ⇒ τ = 2/b