Mark O. answered 11/25/16
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Hi Alex,
Let me first try to draw a picture of this problem:
O beacon
/|
/ |
/ |
r /θ | L
/ |
/ |
___________________________ /___ |______________ shore line
Let me first try to draw a picture of this problem:
O beacon
/|
/ |
/ |
r /θ | L
/ |
/ |
___________________________ /___ |______________ shore line
x
Now, L is the constant distance of the beacon from the straight shore. r is the path length of the current beam of light to the shore. Let θ be the instantaneous angle in radians that the light path makes with the vertical to the shore. Also, let x be the horizontal leg of this right triangle.
Now, L is the constant distance of the beacon from the straight shore. r is the path length of the current beam of light to the shore. Let θ be the instantaneous angle in radians that the light path makes with the vertical to the shore. Also, let x be the horizontal leg of this right triangle.
Let's write tanθ = x/L
Let's take the time derivative of each side of this last equation.
d/dt (tanθ) = d/dt (x/L)
For the left-hand side, d/dt (tanθ) = (dθ/dt)sec2θ, using the chain rule, understanding that θ is a time-dependent function.
For the right-hand side, we realize that L is a constant, so it can be pulled outside the derivative operator, and we can write: d/dt (x/L) = (1/L) dx/dt = v/L where v is the velocity that the light beam moves along the shore.
We now have
(dθ/dt)sec2θ = v/L
dθ/dt is the constant angular velocity, which we normally denote by ω. So, we can now write
ω sec2θ = v/L
Solving for the velocity, we get
v = ωL sec2θ
We know that
ω = 3 rad/min
L = 10 km
θ = pi/3 rad = 60 deg at the instant of interest.
So, the speed that the light beam moves along the shore at this instant is
v = (3 rad/min)(10 km)sec2(60 deg) = (3 rad/min)(10 km)(22) = (3 rad/min)(10 km)(4) = 120 km/min
This is what I get.