The equation of motion for the pendulum:
d2θdt2=−glsinθ, θ(0)=α, dθ(0)dt=0.\frac{d^2\theta}{dt^2}=-\frac{g}{l}sin\theta, \;\;\theta (0)=\alpha,\;\;\frac{d\theta (0)}{dt}=0.dt2d2θ=−lgsinθ,θ(0)=α,dtdθ(0)=0.
For small angles θ\thetaθ we can use the approximation sinθ=θ.sin\theta=\theta.sinθ=θ.
Thus, the solution of the initial value problem
d2θdt=−glθ, θ(0)=α, dθdt=0\frac{d^2\theta}{dt}=-\frac{g}{l}\theta,\;\; \theta (0)=\alpha,\;\;\frac{d\theta}{dt}=0dtd2θ=−lgθ,θ(0)=α,dtdθ=0
is θ=αcos(glt).\theta=\alpha cos(\sqrt{\frac{g}{l}}t).θ=αcos(lgt).
v(t)=dθdt=−αglsin(glt)v(t)=\frac{d\theta}{dt}=-\alpha\sqrt{\frac{g}{l}}sin(\sqrt{\frac{g}{l}}t)v(t)=dtdθ=−αlgsin(lgt).
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