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An electric field is expressed as vec E ...

An electric field is expressed as `vec E = 2 hat i + 3 hat j`. Find the potential difference `(V_A - V_B)` between two points `A` and `B` whose position vectors are given by `r_A = hat i + 2 hat j and r_B = 2 hat i + hat j + 3 hat k`.

A

`-1 V`

B

1 V

C

2 V

D

3 V

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To solve the problem of finding the potential difference \( V_A - V_B \) between two points \( A \) and \( B \) in an electric field, we can follow these steps: ### Step 1: Understand the Electric Field and Position Vectors We are given the electric field: \[ \vec{E} = 2 \hat{i} + 3 \hat{j} \] and the position vectors: \[ \vec{r_A} = \hat{i} + 2 \hat{j} \quad \text{and} \quad \vec{r_B} = 2 \hat{i} + \hat{j} + 3 \hat{k} \] ### Step 2: Set Up the Potential Difference Formula The potential difference \( V_A - V_B \) can be calculated using the relation: \[ V_B - V_A = -\int_{\vec{r_A}}^{\vec{r_B}} \vec{E} \cdot d\vec{l} \] This means we need to integrate the electric field along the path from point \( A \) to point \( B \). ### Step 3: Define the Path of Integration The differential path element \( d\vec{l} \) can be expressed in terms of its components: \[ d\vec{l} = dx \hat{i} + dy \hat{j} \] ### Step 4: Set Up the Integral We need to evaluate the integral: \[ V_B - V_A = -\int_{\vec{r_A}}^{\vec{r_B}} (2 \hat{i} + 3 \hat{j}) \cdot (dx \hat{i} + dy \hat{j}) \] This simplifies to: \[ V_B - V_A = -\int_{\vec{r_A}}^{\vec{r_B}} (2dx + 3dy) \] ### Step 5: Determine the Limits of Integration From the position vectors: - For point \( A \) at \( (1, 2) \) (i.e., \( x = 1, y = 2 \)) - For point \( B \) at \( (2, 1) \) (i.e., \( x = 2, y = 1 \)) ### Step 6: Evaluate the Integral We can break the integral into two parts: 1. Integrate with respect to \( x \) from \( 1 \) to \( 2 \): \[ -\int_{1}^{2} 2 \, dx = -2[x]_{1}^{2} = -2(2 - 1) = -2 \] 2. Integrate with respect to \( y \) from \( 2 \) to \( 1 \): \[ -\int_{2}^{1} 3 \, dy = -3[y]_{2}^{1} = -3(1 - 2) = 3 \] ### Step 7: Combine the Results Now we combine the results of the two integrals: \[ V_B - V_A = -2 + 3 = 1 \] ### Step 8: Finalize the Potential Difference Thus, we have: \[ V_A - V_B = - (V_B - V_A) = -1 \text{ Volt} \] ### Conclusion The potential difference between points \( A \) and \( B \) is: \[ V_A - V_B = -1 \text{ Volt} \]

To solve the problem of finding the potential difference \( V_A - V_B \) between two points \( A \) and \( B \) in an electric field, we can follow these steps: ### Step 1: Understand the Electric Field and Position Vectors We are given the electric field: \[ \vec{E} = 2 \hat{i} + 3 \hat{j} \] and the position vectors: ...
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