How can the range of a projectile fired at an angle up a hill be calculated?

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the following problem is from the 5th edition of Thorton and Marion's "Classical Dynamics"
ch.2 problem 14 p.92

Homework Statement
A projectile is fired with initial speed v_0 at an elevation angle of alpha up a hill of slope beta (alpha > beta).

(a) how far up the hill will the projectile land?
(b) at what angle alpha will the range be a maximum?
(c) what is the maximum angle?

The attempt at a solution
apparently this has been a stumper in former classical mechanics classes, but here was as far as i got:

i broke down the components of the forces into x and y
x-component:
a_x=0 integrating -->
v_x = v_0 cos(beta) integrating -->
x = v_0 t cos(beta)

a_y = -g integrating -->
v_y = -gt + v_0 sin (alpha - beta) integrating -->
y = ( -gt^2 / 2 ) + v_0 sin (alpha - beta)


the answer in the back of the book for part (a) is:
d = (2 v_0^2 cos(alpha) sin(alpha-beta) ) / (g cos^2(beta))

any idea how to get from the components to the answer?
 
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Hint: The distance is the magnitude of the position vector.
 
Hootenanny said:
Hint: The distance is the magnitude of the position vector.

I too am having trouble with this problem. In the book, they use Taylor expansions in order to find the flight time T and put in back into the range equation. However, they have the luxury of letting y = 0 because the trajectory is a simple parabola. We don't have the same situation here. y doesn't equal zero, y = beta*range.
 
I have no idea how we're supposed to get things like cos(\beta)
 
To solve this, I first used the units to work out that a= m* a/m, i.e. t=z/λ. This would allow you to determine the time duration within an interval section by section and then add this to the previous ones to obtain the age of the respective layer. However, this would require a constant thickness per year for each interval. However, since this is most likely not the case, my next consideration was that the age must be the integral of a 1/λ(z) function, which I cannot model.
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