Let us write the equations of motion of a snowball, thrown at angle θ, with initial speed v0:
x=v0cosθ⋅t , y=y0+v0sinθ⋅t−2gt2 .
When the snowball reaches the target, the height is the same as initial, hence y0=y0+v0sinθ⋅t−2gt2 , from where v0sinθ=2gt, and t=g2v0sinθ. Plugging in the last expression into equation for x, obtain x=gv022sinθcosθ=gv02sin2θ (using trigonometric identity sin2x=2sinxcosx).
If we have two snowballs, thrown at different angles θ1,θ2 with the same initial speed v0, their horizontal positions must be equal , hence gv02sin2θ1=gv02sin2θ2, from where sin2θ1=sin2θ2. This condition must hold for two angles, to implement out snowball fight strategy. The condition holds when θ2=2π−θ1, so we need to throw the second snowball at an angle 90∘−66∘=24∘ above the horizontal.
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