If you place a rabbit uniformly at random on a circular table with radius r = 1 meter and it moves straight 1 meter in a random direction, what is the chance it won't fall off?
Round off your answer to 3 decimal places.
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@Mark Hennings shouldn't the conditional probability that the rabbit heads off in the segment RAB be 2 ∗ π 1 \acos ( r / 2 ) ? What am i missing?
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The acute angle ORA is cos − 1 2 1 r . The probability is twice the acute angle divided by 2 π .
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@Mark Hennings Oh silly me! yeah i got it, thanks!
lets define a function that has the following properties;
p(r) equals to the area contained inside if the sub-circle with radius r divided by the entire area of the table.
here p(r) is the probability that the rabbit is put inside of a circle with radius r<=1, however we want to calculate the chance if the rabbit is put on a circumference of thickness d r → 0 .
P ( r ) = p ( r ) − p ( r − d r )
P ( r ) = π R 2 π r 2 − π R 2 π ( r − d r ) 2
P ( r ) = π R 2 π 2 r d r = 2 r d r
Now the interesting part (
Geometry part of this problem
)
using the cosine law we can simply yield that ϕ = a c o s ( 2 r )
the problem here that if the rabbit was put inside he can choose a wrong direction and fall off the table so
the chance that this idiot choose the right direction is C ( r ) = ϕ ( r ) / π
and the total chance that he wont fall off is the sum of C ( r ) ∗ P ( r )
So what we want to calculate is the chance he still be on the table W so
W = ∫ 0 1 ( π 2 r a c o s ( 2 r ) d r ) = ∗ ∗ 0 . 3 9 1 ∗ ∗
In the integral its arccos not racos
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Suppose that the rabbit is at a distance r metres from the centre O of the table. The rabbit will not fall off provided that it heads of in a direction within the minor segment R A B . The (conditional) probability of this happening is π 1 cos − 1 ( 2 1 r ) .
Thus the probability that the rabbit does not fall off the table is π 1 ∫ 0 1 π 1 cos − 1 ( 2 1 r ) 2 π r d r = = = = = = π 2 ∫ 0 1 r cos − 1 ( 2 1 r ) d r π 2 [ 2 1 r 2 cos − 1 ( 2 1 r ) ] 0 1 + π 1 ∫ 0 1 4 − r 2 r 2 d r 3 1 + π 1 ∫ 0 6 1 π 2 cos θ 4 sin 2 θ 2 cos θ d θ 3 1 + π 2 ∫ 0 6 1 π ( 1 − cos 2 θ ) d θ 3 1 + π 2 [ θ − 2 1 sin 2 θ ] 0 6 1 π 3 2 − 2 π 3 = 0 . 3 9 1