Solveeit Logo

Question

Question: A river is flowing with speed $v_0$ m/s. Width of the river is $d$. A boat starts from point $P$. Bo...

A river is flowing with speed v0v_0 m/s. Width of the river is dd. A boat starts from point PP. Boat crosses the river such that its velocity w.r.t. river is always directed towards a fix point QQ which is directly opposite to point PP. Find drift of the boat if speed of boat in still water is also v0v_0.

A

d3\frac{d}{3}

B

d2\frac{d}{2}

C

d4\frac{d}{4}

D

d3\frac{d}{\sqrt{3}}

Answer

d2\frac{d}{2}

Explanation

Solution

Let the river flow along the x-axis with velocity vr=v0i^\vec{v}_r = v_0 \hat{i}. The width of the river is dd along the y-axis. Let the starting point PP be at the origin (0,0)(0,0) and the destination point QQ be at (0,d)(0,d).

The velocity of the boat relative to the river, vbr\vec{v}_{br}, has a magnitude of v0v_0 and is always directed towards point QQ. If the boat is at position (x,y)(x,y), the vector from the boat to QQ is (x,dy)(-x, d-y). Thus, the velocity of the boat relative to the river is: vbr=v0(x,dy)(x)2+(dy)2=v0(xx2+(dy)2i^+dyx2+(dy)2j^)\vec{v}_{br} = v_0 \frac{(-x, d-y)}{\sqrt{(-x)^2 + (d-y)^2}} = v_0 \left( \frac{-x}{\sqrt{x^2 + (d-y)^2}} \hat{i} + \frac{d-y}{\sqrt{x^2 + (d-y)^2}} \hat{j} \right)

The velocity of the boat relative to the ground is vb=vbr+vr\vec{v}_b = \vec{v}_{br} + \vec{v}_r. vb=v0(xx2+(dy)2i^+dyx2+(dy)2j^)+v0i^\vec{v}_b = v_0 \left( \frac{-x}{\sqrt{x^2 + (d-y)^2}} \hat{i} + \frac{d-y}{\sqrt{x^2 + (d-y)^2}} \hat{j} \right) + v_0 \hat{i} vb=v0(1xx2+(dy)2)i^+v0dyx2+(dy)2j^\vec{v}_b = v_0 \left( 1 - \frac{x}{\sqrt{x^2 + (d-y)^2}} \right) \hat{i} + v_0 \frac{d-y}{\sqrt{x^2 + (d-y)^2}} \hat{j}

Let vx=dxdtv_x = \frac{dx}{dt} and vy=dydtv_y = \frac{dy}{dt}. We have: dxdt=v0(1xx2+(dy)2)\frac{dx}{dt} = v_0 \left( 1 - \frac{x}{\sqrt{x^2 + (d-y)^2}} \right) dydt=v0dyx2+(dy)2\frac{dy}{dt} = v_0 \frac{d-y}{\sqrt{x^2 + (d-y)^2}}

To find the path of the boat, we can find the ratio dxdy\frac{dx}{dy}: dxdy=vxvy=v0(1xx2+(dy)2)v0dyx2+(dy)2=x2+(dy)2xdy\frac{dx}{dy} = \frac{v_x}{v_y} = \frac{v_0 \left( 1 - \frac{x}{\sqrt{x^2 + (d-y)^2}} \right)}{v_0 \frac{d-y}{\sqrt{x^2 + (d-y)^2}}} = \frac{\sqrt{x^2 + (d-y)^2} - x}{d-y} Let u=dyu = d-y. Then y=duy = d-u, so dydu=1\frac{dy}{du} = -1, which means dxdu=dxdydydu=dxdy\frac{dx}{du} = \frac{dx}{dy} \frac{dy}{du} = -\frac{dx}{dy}. The differential equation becomes: dxdu=x2+u2xu-\frac{dx}{du} = \frac{\sqrt{x^2+u^2} - x}{u} dxdu=xx2+u2u=xux2+u2u\frac{dx}{du} = \frac{x - \sqrt{x^2+u^2}}{u} = \frac{x}{u} - \frac{\sqrt{x^2+u^2}}{u} This is a homogeneous differential equation. Let x=vux = vu, so dxdu=v+udvdu\frac{dx}{du} = v + u\frac{dv}{du}. v+udvdu=vuu(vu)2+u2uv + u\frac{dv}{du} = \frac{vu}{u} - \frac{\sqrt{(vu)^2+u^2}}{u} v+udvdu=vuv2+1uv + u\frac{dv}{du} = v - \frac{u\sqrt{v^2+1}}{u} udvdu=v2+1u\frac{dv}{du} = -\sqrt{v^2+1} dvv2+1=duu\frac{dv}{\sqrt{v^2+1}} = -\frac{du}{u} Integrating both sides: dvv2+1=duu\int \frac{dv}{\sqrt{v^2+1}} = -\int \frac{du}{u} lnv+v2+1=lnu+C1\ln|v+\sqrt{v^2+1}| = -\ln|u| + C_1 lnv+v2+1=ln(1u)+C1\ln|v+\sqrt{v^2+1}| = \ln\left(\frac{1}{|u|}\right) + C_1 v+v2+1=Au(where A=eC1)v+\sqrt{v^2+1} = \frac{A}{u} \quad (\text{where } A = e^{C_1}) Substitute back v=x/uv = x/u: xu+x2u2+1=Au\frac{x}{u} + \sqrt{\frac{x^2}{u^2}+1} = \frac{A}{u} xu+x2+u2u=Au\frac{x}{u} + \frac{\sqrt{x^2+u^2}}{u} = \frac{A}{u} x+x2+u2=Ax + \sqrt{x^2+u^2} = A The boat starts at P(0,0)P(0,0), so x=0x=0 when y=0y=0. When y=0y=0, u=d0=du = d-0 = d. Substituting x=0x=0 and u=du=d: 0+02+d2=A    A=d0 + \sqrt{0^2+d^2} = A \implies A = d So the equation of the boat's path is: x+x2+u2=dx + \sqrt{x^2+u^2} = d Substitute u=dyu=d-y: x+x2+(dy)2=dx + \sqrt{x^2+(d-y)^2} = d The drift is the value of xx when the boat reaches the other bank, i.e., when y=dy=d. When y=dy=d, u=dd=0u = d-d = 0. x+x2+02=dx + \sqrt{x^2+0^2} = d x+x2=dx + \sqrt{x^2} = d Since the boat moves in the positive x direction, x>0x>0, so x2=x\sqrt{x^2}=x. x+x=dx + x = d 2x=d2x = d x=d2x = \frac{d}{2} The drift of the boat is d2\frac{d}{2}.