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Question: Average torque on a projectile of mass m, initial speed u and angle of projection θ between initial ...

Average torque on a projectile of mass m, initial speed u and angle of projection θ between initial and final positions P and Q as shown in the figure about the point of projection is:
A. mu2sin2θ2\dfrac{{m{u^2}\sin 2\theta }}{2}
B. mu2cosθm{u^2}\cos \theta
C. u2sinθ{u^2}\sin \theta
D. mu2cosθ2\dfrac{{m{u^2}\cos \theta }}{2}

Explanation

Solution

We should know the definition of torque, angular momentum etc.
We should know the relationship between angular momentum and torque.

Complete step by step answer:
Average Torque would just be the time, average of that varying quantity averaged over the time it takes to complete a revolution. The basic equation between torque and angular momentum is, τ.Δt = ΔL\tau .\Delta {\text{t = }}\Delta {\text{L}}

We know that the basic equation between torque and angular momentum is,

τ.Δt = ΔL\tau .\Delta {\text{t = }}\Delta {\text{L}}

And angular momentum is the quantity of rotation of a body, which is the product of its moment of inertia and its angular velocity.

Torque is a force that caused machinery, etc. to turn (rotate)\left( {rotate} \right)

We know from basic equation that,

τ.Δt = ΔL\tau .\Delta {\text{t = }}\Delta {\text{L}}

Δt = 2usinθg[u=speed,θ=angle  of projection] ΔL=[LfLi]  [Lf=find  momentum]  [Li=initial  momentum]  \Delta t{\text{ = }}\dfrac{{2u\sin \theta }}{g}\left[ {u = speed,\theta = angle\;{\text{of projection}}} \right] \\\ \Delta L = \left[ {{L_f} - {L_i}} \right]\;\left[ {{L_f} = find\;{\text{momentum}}} \right]\;\left[ {{L_i} = initial\;{\text{momentum}}} \right] \\\

Initial momentum is zero as it starts form a static point thus,

ΔL=(Lf)=m.usinθ×R mvsinθ×u2sin2θg mu3sinθ.sin2θg  \because \Delta L = \left( {{L_f}} \right) = m.u\sin \theta \times R \\\ mv\sin \theta \times \dfrac{{{u^2}\sin 2\theta }}{g} \\\ \dfrac{{m{u^3}\sin \theta .\sin 2\theta }}{g} \\\
Therefore we know that,
τag=ΔLΔt mu3sinθ.sin2θg.2usinθg=mu2sin2θ2  {\tau _{ag}} = \dfrac{{\Delta L}}{{\Delta t}} \\\ \dfrac{{m{u^3}\sin \theta .\sin 2\theta }}{{g.\dfrac{{2u\sin \theta }}{g}}} = \dfrac{{m{u^2}\sin 2\theta }}{2} \\\

So, the correct answer is “Option A”.

Note:
We should take care of substitutions of different equations in one.
We should remember all basic equations.
We should make sure to avoid substitution errors.