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Question: A boat moves relative to water with a velocity half of the river flow velocity if the angle from the...

A boat moves relative to water with a velocity half of the river flow velocity if the angle from the direction of flow with which boat must move relative to stream directly to minimize drift is 2×πn\dfrac{{2 \times \pi }}{n}, then n is:
(A)\left( A \right) 1
(B)\left( B \right) 0
(C)\left( C \right) 4
(D)\left( D \right) 3

Explanation

Solution

Hint – Draw the diagrammatic representation, with the velocity of the river be u (moving in R.H.S direction) and the velocity of the boat be v making an angle θ\theta with perpendicular joining two ends of the rivers or an angle of 90o+θ{90^o} + \theta with the initial velocity of the river. Let the width of the river be (d) meters, resolve the velocity into its components and use the concept that drifting distance is equal to the time taken by the boat and the horizontal component of the velocity. This will help approaching the problem.

Complete step-by-step answer:

Let the velocity of the river be u (moving in R.H.S direction) and the velocity of the boat be v as shown in the figure.
Let the boat start moving in the river from point A, it did not reach to point B which is vertically opposite to point A because of the velocity of the river.
To minimize the drift we have to row the boat at an angle θ\theta with the vertical as shown in the figure.
So the angle (θ)\left( {\theta '} \right) boat makes with the positive direction of x axis is, θ=\theta ' = 900+θ{90^0} + \theta ............. (1)
Let the width of the river be (d).
Now the components of the velocity in the x and y axis are vsinθv\sin \theta and vcosθv\cos \theta as shown in the figure.
So the vertical velocity component is Vy=vcosθ{V_y} = v\cos \theta
And the horizontal velocity component is Vx=uvsinθ{V_x} = u - v\sin \theta
Let the time taken by the boat to cross the river be (t).
So the time taken by the boat is = t=dVyt = \dfrac{d}{{{V_y}}}
t=dvcosθ\Rightarrow t = \dfrac{d}{{v\cos \theta }}....................... (2)
Now let the boat be drifted by x units as shown in the figure.
So this drifting distance is equal to the time taken by the boat and the horizontal component of the velocity.
x=t.Vx\Rightarrow x = t.{V_x}
x=dvcosθ(uvsinθ)\Rightarrow x = \dfrac{d}{{v\cos \theta }}\left( {u - v\sin \theta } \right)
Now we have to minimize this drift and find out the value of the angle the boat makes with the positive direction of the x axis.
So differentiate it w.r.t θ\theta and equate to zero we have,
ddθx=ddθ[dvcosθ(uvsinθ)]=ddθ[udvcosθ]ddθ(dsinθcosθ)=0\Rightarrow \dfrac{d}{{d\theta }}x = \dfrac{d}{{d\theta }}\left[ {\dfrac{d}{{v\cos \theta }}\left( {u - v\sin \theta } \right)} \right] = \dfrac{d}{{d\theta }}\left[ {\dfrac{{ud}}{{v\cos \theta }}} \right] - \dfrac{d}{{d\theta }}\left( {d\dfrac{{\sin \theta }}{{\cos \theta }}} \right) = 0
Now as we know that 1cosθ=secθ and sinθcosθ=tanθ\dfrac{1}{{\cos \theta }} = \sec \theta {\text{ and }}\dfrac{{\sin \theta }}{{\cos \theta }} = \tan \theta so we have,
ddθx=ddθ[udsecθv]ddθ(dtanθ)=0\Rightarrow \dfrac{d}{{d\theta }}x = \dfrac{d}{{d\theta }}\left[ {\dfrac{{ud\sec \theta }}{v}} \right] - \dfrac{d}{{d\theta }}\left( {d\tan \theta } \right) = 0
Now differentiate it according to property ddθsecθ=secθtanθ and ddθtanθ=sec2θ\dfrac{d}{{d\theta }}\sec \theta = \sec \theta \tan \theta {\text{ and }}\dfrac{d}{{d\theta }}\tan \theta = {\sec ^2}\theta so we have,
ddθx=udvsecθtanθdsec2θ=0\Rightarrow \dfrac{d}{{d\theta }}x = \dfrac{{ud}}{v}\sec \theta \tan \theta - d{\sec ^2}\theta = 0
Now simplify this we have,
udvsecθtanθ=dsec2θ\Rightarrow \dfrac{{ud}}{v}\sec \theta \tan \theta = d{\sec ^2}\theta
uvtanθ=secθ\Rightarrow \dfrac{u}{v}\tan \theta = \sec \theta
uvsinθcosθ=1cosθ\Rightarrow \dfrac{u}{v}\dfrac{{\sin \theta }}{{\cos \theta }} = \dfrac{1}{{\cos \theta }}
sinθ=vu\Rightarrow \sin \theta = \dfrac{v}{u}
θ=sin1(vu)\Rightarrow \theta = {\sin ^{ - 1}}\left( {\dfrac{v}{u}} \right).................... (2)
Now it is given that the velocity of the boat is half of the velocity of the river.
v=12u\Rightarrow v = \dfrac{1}{2}u
So substitute this value in equation (2) we have,
θ=sin1(12uu)=sin1(12)=sin1(sin300)=300\Rightarrow \theta = {\sin ^{ - 1}}\left( {\dfrac{{\dfrac{1}{2}u}}{u}} \right) = {\sin ^{ - 1}}\left( {\dfrac{1}{2}} \right) = {\sin ^{ - 1}}\left( {\sin {{30}^0}} \right) = {30^0}
Now from equation (1) we have,
θ=90o+30o=120o\Rightarrow \theta ' = {90^o} + {30^o} = {120^o}
Now convert this into radian by multiplying π1800\dfrac{\pi }{{{{180}^0}}} so we have,
θ=120o×π180o=2×π3\Rightarrow \theta ' = {120^o} \times \dfrac{\pi }{{{{180}^o}}} = \dfrac{{2 \times \pi }}{3}
Now compare this drift with the given drift we have,
2×πn=2×π3\Rightarrow \dfrac{{2 \times \pi }}{n} = \dfrac{{2 \times \pi }}{3}
So on comparing n = 3.
So this is the required answer.

Hence option (D) is the correct answer.

Note – Since the drift has to be minimized therefore we have differentiated the drifting distance w.r.t θ\theta and equate to zero. This gives the value of θ\theta in terms of the velocities of boat and the river. Using the specific relation between speed of boat and the river θ\theta can be obtained. Now we have computed 90o+θ{90^o} + \theta , because the question asks that the angle from the direction of flow with which boat must move relative to stream to minimize drift.