Problem: On a straight shoreline there is a tree and exactly opposite
it,
Solution: Here's how the situation looks like.
We need some mathematical description of this situation. The important things
are the ray whose position is given uniquely by its direction and the light
spot, whose position changes along the shore. Thus we introduce two
variables as functions of time. One will be the position of the light spot
This choice is reasonable for two reasons. First, it allows us to express important facts from our problem as derivatives, namely we know the rate of change of the angle and we are asked to provide the speed of the light spot, that is, the rate of change of its position. Thus we see that we need to relate two rates of change, which is another confirmation that our choice of variables was reasonable.
If we want to relate rates of change, that is, derivatives of two functions, we first have to relate the functions themselves. This is rather simple, from the right-angle triangle in the picture we have
Both sides of this equality are in fact functions of time, so we can differentiate them and obtain an equality again, we do not forget to use the chain rule on the right.
Of course, this equation only works for angles which make the light shine
toward the shore, that is, for angles from the interval
and its
shifts by
The speed of rotation on the right is given by the fact that the light makes
a whole circle, that is, the angle
Again, this only works for angles as above. Note that this formula behaves in
a way that agrees with our common sense. The speed of the light spot is
smallest exactly opposite the lighthouse (when the angle is zero) and the
further we go from the tree, the faster the spot goes. It remains to find out
the speed at the place where we stand. There the corresponding angle is
This makes about