Problem:
A car travels due east at 32β mile per minute on a long, straight road. At the same time, a circular storm, whose radius is 51 miles, moves southeast at 21β2β mile per minute. At time t=0, the center of the storm is 110 miles due north of the car. At time t=t1β minutes, the car enters the storm circle, and at time t=t2β minutes, the car leaves the storm circle. Find 21β(t1β+t2β).
Solution:
Let r be the radius of the storm, d be the distance from the center of the storm to the car at time t=0,c be the speed of the car, and s2β be the speed of the storm. Set up a coordinate system so that, at t=0, the storm center is at (0,d), and the car is at the origin, moving along the positive x-axis. At any time t, the car is at (ct,0) and the storm center is at (st,dβst). When the car is entering or leaving the storm circle, the distance between these two points is r. In other words, t1β and t2β are the solutions to
(ctβst)2+(dβst)2=r2
which can be rewritten as ((cβs)2+s2)t2β(2ds)t+(d2βr2)=0. The sum of the two roots of this quadratic equation is
t1β+t2β=(cβs)2+s22dsβ
Now use the given data c=32β,d=110, and s=21β to find that
The discriminant 4d2s2β4(d2βr2)((cβs)2+s2) of the quadratic equation is nonnegative in this case, therefore t1β and t2β are real. The answer is otherwise independent of r.
OR
Make the storm center the origin O of a coordinate system that has its positive x-axis pointing east. At time t=0, the car is at C=(0,β110). Each minute thereafter, its position relative to the storm center is shifted by the velocity vector
(2/3,0)β(1/2,β1/2)=(1/6,1/2)
due to the combined motion of the car and storm, respectively. The resulting linear path of the car intersects the storm along a chord of the circle, whose midpoint M is reached at time t=21β(t1β+t2β). Because angle CMO is right, and tanβ OCM is 31β, it follows that CM=COcosβ OCM=110β 10β3β=3310β. To find the time it takes for the car to reach M, divide this distance by the relative speed of the car, which is 61β10β. It follows that