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Let V(0) be the potential at the origin ...

Let `V_(0)` be the potential at the origin in an electric field `vecE=E_(x)hati+E_(y)hatj`. The potential at the point `(x,y)` is

A

`V_(@)+xE_(x)+yE_(y)`

B

`V_(@)+xE_(x)-yE_(y)`

C

`V_(@)-xE_(x)-yE_(y)`

D

`sqrt((x^(2)+y^(2)))sqrt((E_(x)^(2)+E_(y)^(2)))-V_(@)`

Text Solution

AI Generated Solution

The correct Answer is:
To find the potential at the point \((x, y)\) in an electric field given by \(\vec{E} = E_x \hat{i} + E_y \hat{j}\), we can follow these steps: ### Step-by-Step Solution 1. **Understand the Relationship Between Electric Field and Potential**: The electric potential \(V\) at a point in an electric field is related to the electric field \(\vec{E}\) by the equation: \[ V_P - V_0 = -\int_{0}^{P} \vec{E} \cdot d\vec{r} \] where \(V_P\) is the potential at point \(P\), \(V_0\) is the potential at the origin, and \(d\vec{r}\) is the differential displacement vector. 2. **Define the Position Vector**: The position vector of point \(P\) can be expressed as: \[ \vec{r} = x \hat{i} + y \hat{j} \] 3. **Calculate the Change in Potential**: The change in potential from the origin to point \(P\) can be expressed as: \[ V_P - V_0 = -\int_{0}^{P} \vec{E} \cdot d\vec{r} \] Here, we can express \(\vec{E}\) as: \[ \vec{E} = E_x \hat{i} + E_y \hat{j} \] 4. **Evaluate the Dot Product**: The differential displacement \(d\vec{r}\) can be expressed as: \[ d\vec{r} = dx \hat{i} + dy \hat{j} \] Therefore, the dot product \(\vec{E} \cdot d\vec{r}\) becomes: \[ \vec{E} \cdot d\vec{r} = (E_x \hat{i} + E_y \hat{j}) \cdot (dx \hat{i} + dy \hat{j}) = E_x dx + E_y dy \] 5. **Integrate to Find the Potential**: Now we can integrate: \[ V_P - V_0 = -\int_{0}^{P} (E_x dx + E_y dy) \] This can be separated into two integrals: \[ V_P - V_0 = -\left( \int_{0}^{x} E_x dx + \int_{0}^{y} E_y dy \right) \] 6. **Evaluate the Integrals**: Assuming \(E_x\) and \(E_y\) are constant (or can be treated as such over the path), we can evaluate the integrals: \[ V_P - V_0 = -\left( E_x x + E_y y \right) \] 7. **Express the Potential at Point \(P\)**: Rearranging gives us the potential at point \(P\): \[ V_P = V_0 - (E_x x + E_y y) \] ### Final Answer Thus, the potential at the point \((x, y)\) is: \[ V_P = V_0 - (E_x x + E_y y) \]
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