
Bradford T. answered 01/01/21
MS in Electrical Engineering with 40+ years as an Engineer
G
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|θ\
.3| \
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R x P
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dx/dt = -1500 mi/s
tan(θ) = x/.3
Take derivative of both sides
sec2(θ) dθ/dt = (1/.3)dx/dt
dθ/dt = (1/,3)(1/sec2(θ))dx/dt = (1/.3)cos2(θ) dx/dt
when the masenko beam is .4 mi from Raditz, it forms a .3-.4-.5 triangle, so cos(θ) = .3/.5
dθ/dt = (1/.3)(.3/.5)2(-1500) = (.3/.25)(-1500) = -1800 radians/sec (decreasing)
The kamehamaha velocity is not needed