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A solid sphere of radius R is charged un...

A solid sphere of radius `R` is charged uniformly. The electrostatic potential `V` is plotted as a function of distance `r` from the centre of th sphere. Which of the following best represents the resulting curve?

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To solve the problem of determining the shape of the electrostatic potential \( V \) as a function of distance \( r \) from the center of a uniformly charged solid sphere, we will analyze the potential in three distinct regions: outside the sphere, at the surface, and inside the sphere. ### Step-by-Step Solution: 1. **Understanding the Regions**: - We have a solid sphere of radius \( R \) that is uniformly charged with total charge \( Q \). - We need to analyze the potential \( V \) for three cases: - Case 1: \( r > R \) (outside the sphere) - Case 2: \( r = R \) (at the surface of the sphere) - Case 3: \( r < R \) (inside the sphere) 2. **Case 1: Outside the Sphere (\( r > R \))**: - The potential \( V \) at a distance \( r \) from the center of the sphere is given by the formula: \[ V(r) = \frac{KQ}{r} \] - Here, \( K \) is the electrostatic constant. - This equation represents a hyperbolic relationship, where the potential decreases as \( r \) increases. 3. **Case 2: At the Surface of the Sphere (\( r = R \))**: - At the surface, we can substitute \( r = R \) into the equation: \[ V(R) = \frac{KQ}{R} \] - This gives us the potential at the surface of the sphere. 4. **Case 3: Inside the Sphere (\( r < R \))**: - The potential inside a uniformly charged solid sphere is given by: \[ V(r) = \frac{KQ}{2R} \left( 3 - \frac{r^2}{R^2} \right) \] - This equation shows that the potential is a quadratic function of \( r \) and opens downward, indicating that as \( r \) approaches \( R \), the potential approaches \( \frac{KQ}{R} \). 5. **Combining the Results**: - For \( r < R \), the potential is a downward-opening parabola. - At \( r = R \), the potential reaches a maximum value \( \frac{KQ}{R} \). - For \( r > R \), the potential decreases hyperbolically as \( \frac{KQ}{r} \). 6. **Graph Representation**: - The graph of \( V \) as a function of \( r \) will show: - A downward parabola for \( r < R \). - A constant value at \( r = R \). - A hyperbolic decrease for \( r > R \). ### Conclusion: The best representation of the resulting curve for the electrostatic potential \( V \) as a function of distance \( r \) from the center of the sphere is a combination of a downward parabola for \( r < R \) and a hyperbola for \( r > R \). The correct option is the one that reflects this behavior.

To solve the problem of determining the shape of the electrostatic potential \( V \) as a function of distance \( r \) from the center of a uniformly charged solid sphere, we will analyze the potential in three distinct regions: outside the sphere, at the surface, and inside the sphere. ### Step-by-Step Solution: 1. **Understanding the Regions**: - We have a solid sphere of radius \( R \) that is uniformly charged with total charge \( Q \). - We need to analyze the potential \( V \) for three cases: - Case 1: \( r > R \) (outside the sphere) ...
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