Jason L. answered 06/03/22
B.S. Degree in Physics with 4 Years of Teaching Experience
Assuming the small angle approximation (oscillations ≤ 15°), the damped pendulum’s position can be modeled with the equation, X(t) = e^(-αt)*(Asin(wt)+Bcos(wt)), where X(t) is the amplitude of the oscillation at time, t, and w is the angular frequency, so w = √(g/L). The period for 1 oscillation is 2pi/w, so the time for 103 oscillations is 103*(2pi/w), and X(t) after 103 oscillations is X(0)/2. Also, X(0) = e^(-α0)*(Asin(w0)+Bcos(w0)) = 1*(A*0 + B*1) = B. So, now substituting in the time of 103 oscillations gives X(103*(2pi/w)) = e^(-α103*(2pi/w))*(Asin(w103*(2pi/w))+Bcos(w103*(2pi/w))) = e^(-α103*(2pi/w))*(Asin(103*(2pi))+Bcos(103*(2pi))). Now, we can use the fact that sin(n*2pi) = 0 and cos(n*2pi) = 1 for integers, n, to simplify it to: X(103*(2pi/w)) = e^(-α103*(2pi/w))*B. And, since we found earlier that B = X(0) and X(q03*(2pi/w)) = X(0)/2, we can substitute those in to get: X(0)/2 = e^(-α103*(2pi/w))*X(0) canceling X(0) and taking ln of both sides then gives ln(1/2) = -α103*(2pi/w). Using the fact that ln(1/2) = -ln2 and isolating α gives: ln2/(103*(2pi/w)) = α, and since w = √(g/L), we finally get: α = ln2/(103*(2pi/√(g/L))) = ln2/(103*(2pi/√(9.8/0.93))) = 0.00348 Hz.