arthham

JEE Advanced 2019 · Work, Energy and Power

A particle is moved along a path AB-BC-CD-DE-EF-FA, as shown in figure, in presence of a forced F=(αyi+2αxj)N,F = (α y i + 2α x j) N, where x and y are in meter and α=−1Nm−1.α = -1 N m^{-1}. The work done on the particle by this force F will be ___ Joule.

Answer: 0.750.75

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Written solution

Step 1: Define the force vector and the work integral.

The given force vector is:

F⃗=αyi^+2αxj^\vec{F} = \alpha y\hat{i} + 2\alpha x\hat{j}

Substituting α=−1 N m−1\alpha = -1\,\text{N}\,\text{m}^{-1} yields:

F⃗=−yi^−2xj^\vec{F} = -y\hat{i} - 2x\hat{j}

The total work done along the closed path is:

W=∮F⃗⋅dr⃗W = \oint \vec{F} \cdot d\vec{r} W=∮(−y dx−2x dy)W = \oint (-y\,dx - 2x\,dy)

Step 2: Calculate the work done along each segment.

The closed path consists of six segments: ABAB, BCBC, CDCD, DEDE, EFEF, and FAFA.

For segment ABAB from (0,1)(0, 1) to (1,1)(1, 1), y=1y = 1 and dy=0dy = 0:

WAB=∫01−1 dx=−1 JW_{AB} = \int_{0}^{1} -1\,dx = -1\,\text{J}

For segment BCBC from (1,1)(1, 1) to (1,0.5)(1, 0.5), x=1x = 1 and dx=0dx = 0:

WBC=∫10.5−2(1) dy=1 JW_{BC} = \int_{1}^{0.5} -2(1)\,dy = 1\,\text{J}

For segment CDCD from (1,0.5)(1, 0.5) to (0.5,0.5)(0.5, 0.5), y=0.5y = 0.5 and dy=0dy = 0:

WCD=∫10.5−0.5 dx=0.25 JW_{CD} = \int_{1}^{0.5} -0.5\,dx = 0.25\,\text{J}

For segment DEDE from (0.5,0.5)(0.5, 0.5) to (0.5,0)(0.5, 0), x=0.5x = 0.5 and dx=0dx = 0:

WDE=∫0.50−2(0.5) dy=0.5 JW_{DE} = \int_{0.5}^{0} -2(0.5)\,dy = 0.5\,\text{J}

For segment EFEF from (0.5,0)(0.5, 0) to (0,0)(0, 0), y=0y = 0 and dy=0dy = 0:

WEF=∫0.500 dx=0 JW_{EF} = \int_{0.5}^{0} 0\,dx = 0\,\text{J}

For segment FAFA from (0,0)(0, 0) to (0,1)(0, 1), x=0x = 0 and dx=0dx = 0:

WFA=∫01−2(0) dy=0 JW_{FA} = \int_{0}^{1} -2(0)\,dy = 0\,\text{J}

Step 3: Sum the work done over all segments.

W=WAB+WBC+WCD+WDE+WEF+WFAW = W_{AB} + W_{BC} + W_{CD} + W_{DE} + W_{EF} + W_{FA} W=−1+1+0.25+0.5+0+0W = -1 + 1 + 0.25 + 0.5 + 0 + 0 W=0.75 JW = 0.75\,\text{J}

Step 4: Verify using Green's Theorem.

The curl of the force field is:

∂Fy∂x−∂Fx∂y=2α−α=α\frac{\partial F_y}{\partial x} - \frac{\partial F_x}{\partial y} = 2\alpha - \alpha = \alpha

Since the path is traversed clockwise, the work done is:

W=−∬α dA=−αAW = -\iint \alpha\,dA = -\alpha A

The enclosed area AA is:

A=(1×1)−(0.5×0.5)=0.75 m2A = (1 \times 1) - (0.5 \times 0.5) = 0.75\,\text{m}^2

Substituting α=−1 N m−1\alpha = -1\,\text{N}\,\text{m}^{-1} and A=0.75 m2A = 0.75\,\text{m}^2:

W=−(−1)(0.75)=0.75 JW = -(-1)(0.75) = 0.75\,\text{J}

Answer: The work done on the particle by this force is 0.75 Joule.

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