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A body is displaced from origin to (2m, ...

A body is displaced from origin to `(2m, 4m)` under the following two forces:
(a) `F=(2^hati + 6^hatj)N`, a constant force
(b) `F(2x^hati + 3y^(2)hatj)N`
Find work done by the given forces in both cases.

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To find the work done by the given forces in both cases, we will use the formula for work done: \[ W = \int \mathbf{F} \cdot d\mathbf{r} \] where \(\mathbf{F}\) is the force vector and \(d\mathbf{r}\) is the displacement vector. ### Part (a): Constant Force \(\mathbf{F} = (2\hat{i} + 6\hat{j}) \, \text{N}\) 1. **Identify the force vector and displacement vector**: - Force: \(\mathbf{F} = 2\hat{i} + 6\hat{j}\) - Displacement from \((0,0)\) to \((2,4)\): \(d\mathbf{r} = dx \hat{i} + dy \hat{j}\) 2. **Set up the integral for work done**: \[ W = \int_{(0,0)}^{(2,4)} \mathbf{F} \cdot d\mathbf{r} = \int_{0}^{2} \int_{0}^{4} (2\hat{i} + 6\hat{j}) \cdot (dx \hat{i} + dy \hat{j}) \] 3. **Calculate the dot product**: \[ \mathbf{F} \cdot d\mathbf{r} = (2\hat{i} + 6\hat{j}) \cdot (dx \hat{i} + dy \hat{j}) = 2dx + 6dy \] 4. **Integrate**: \[ W = \int_{0}^{2} \int_{0}^{4} (2dx + 6dy) \] This can be separated into two integrals: \[ W = \int_{0}^{2} 2dx + \int_{0}^{4} 6dy \] 5. **Evaluate the integrals**: - For the first integral: \[ \int_{0}^{2} 2dx = 2x \bigg|_{0}^{2} = 2(2) - 2(0) = 4 \] - For the second integral: \[ \int_{0}^{4} 6dy = 6y \bigg|_{0}^{4} = 6(4) - 6(0) = 24 \] 6. **Add the results**: \[ W = 4 + 24 = 28 \, \text{J} \] ### Part (b): Variable Force \(\mathbf{F} = (2x\hat{i} + 3y^2\hat{j}) \, \text{N}\) 1. **Identify the force vector and displacement vector**: - Force: \(\mathbf{F} = 2x\hat{i} + 3y^2\hat{j}\) - Displacement from \((0,0)\) to \((2,4)\): \(d\mathbf{r} = dx \hat{i} + dy \hat{j}\) 2. **Set up the integral for work done**: \[ W = \int_{(0,0)}^{(2,4)} \mathbf{F} \cdot d\mathbf{r} = \int_{0}^{2} \int_{0}^{4} (2x\hat{i} + 3y^2\hat{j}) \cdot (dx \hat{i} + dy \hat{j}) \] 3. **Calculate the dot product**: \[ \mathbf{F} \cdot d\mathbf{r} = (2x\hat{i} + 3y^2\hat{j}) \cdot (dx \hat{i} + dy \hat{j}) = 2x \, dx + 3y^2 \, dy \] 4. **Integrate**: \[ W = \int_{0}^{2} \int_{0}^{4} (2x \, dx + 3y^2 \, dy) \] This can be separated into two integrals: \[ W = \int_{0}^{2} 2x \, dx + \int_{0}^{4} 3y^2 \, dy \] 5. **Evaluate the integrals**: - For the first integral: \[ \int_{0}^{2} 2x \, dx = x^2 \bigg|_{0}^{2} = 2^2 - 0^2 = 4 \] - For the second integral: \[ \int_{0}^{4} 3y^2 \, dy = y^3 \bigg|_{0}^{4} = 4^3 - 0^3 = 64 \] 6. **Add the results**: \[ W = 4 + 64 = 68 \, \text{J} \] ### Final Answers: - Work done by constant force: \(28 \, \text{J}\) - Work done by variable force: \(68 \, \text{J}\)

To find the work done by the given forces in both cases, we will use the formula for work done: \[ W = \int \mathbf{F} \cdot d\mathbf{r} \] where \(\mathbf{F}\) is the force vector and \(d\mathbf{r}\) is the displacement vector. ...
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