Throwing a Javelin (Projectile Motion)

[TopCat]

Homework Statement

An athlete can throw a javelin 60m from a standing position. If he can run 100m at constant velocity in 10s, how far could he hope to throw the javelin while running? Neglect air resistance and the height of the thrower in the interest of simplicity.

Homework Equations

I've found the range to be R(θ) = 2 v0/g sinθ (v0 cosθ + vr)
where v0 is the initial velocity and vr is the velocity of the thrower's initial run.

The Attempt at a Solution

Given the above equation and the premise that the thrower can throw 60m from standing, I solved for v0 using vr=0, R=60, g=9.8, and θ=45° as that is the ideal throwing angle from standing. I found v0 = √(60g).

Next I tried to find the ideal angle to throw at when vr = 10 m/s. I did this by taking solving R'(θ)=0 where R'(θ) is the derivative of the range formula. I found:
R'(θ) = c v0²/2 cos2θ + c vr cosθ = 0 where c = 2 v0/g.

This yielded the equation v0 cos2θ = -vr cosθ. Using an identity for cos2θ, I obtained the following quadratic equation:
2 cos²θ + d cosθ -1 = 0 where d = vr/v0 = 10/√(60g).

Solving for θ I got θ = 0.65 rads = 37°. The book, however, lists 52.3° as the angle, and therefore gets a different value of R than I do. I'm not sure where I went wrong with my logic.

 

[Astronuc]

I haven't look through the detail yet, but assuming that the runner/thrower throws at the same angle as when standing, the runner's velocity adds to the v_x of the javelin, but does not contribute to the vertical velocity.

Make sure the correct angle is calculated for the range (60 m) of the throw from stationary position.

 

[TopCat]

That's kind of what's tying me up. The problem stated nothing about the initial angle thrown, so I made the assumption that the thrower threw at the angle to maximize range. From standstill that's pi/4, and with some added vr, I presumed the ideal angle would change and sought to calculate it and use it to calculate the final range.

 

[Astronuc]

pi/4 is reasonable for max range

http://hyperphysics.phy-astr.gsu.edu/hbase/traj.html#tra12

 

[TopCat]

Okay, so after thinking about this, I've realized the angle clearly should be greater than 45^\circ. This is because the v_x is greater than the v_y when the thrower is running. That being the case, he must throw at a greater angle so that the effective angle thrown at is 45^\circ. Provided that reasoning correct, I have, for maximum range:

v_{0x} = v_{oy}
\Downarrow
v_0 \sin\theta = v_0 \cos\theta + v_r
\Downarrow
\sin\theta - \cos\theta = \frac{v_r}{v_0}

Squaring both sides gives

\sin^2\theta + \cos^2\theta - 2\sin\theta\cos\theta = \frac{v_r^2}{v_0^2}
\Downarrow
\sin2\theta = -\frac{v^2_r}{v^2_0}

However, when I solve that I don't get the angle of 52.3^\circ (I get something ludicrous like -10^\circ). Was my reasoning incorrect?

Also, when I take

R = \frac{2v_0}{g}(v_0 \cos\theta + v_r) \sin\theta

and solve R' = 0 I get 35^\circ as the solution. Where am I going wrong here?