Classical Dynamics of Particles and Systems · Problem 10-10

Dynamics of Rigid Bodies — Marion & Thornton

Physics — Mechanics · projectile-range-change-due-to-rotation

Problem

In the preceding problem, if the range of the projectile is R0′R_0' for the case ω=0\omega = 0, show that the change of range due to the rotation of Earth is ΔR′=2R0′3g⋅ωcos⁡λ(cot⁡1/2α−13tan⁡3/2α)\Delta R' = \sqrt{\frac{2R_0'^3}{g}} \cdot \omega\cos\lambda\left(\cot^{1/2}\alpha - \frac{1}{3}\tan^{3/2}\alpha\right)

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