ELECTRIC POTENTIAL
Electric Potential due to a Point Charge Derivation
Electric Potential due to a Point Charge Derivation |
Work done in bringing test charge `q_0` from B to A.
`W = \int_B^A \vecF.d\vecx`
`W = \int_B^A Fdx cos 180^\circ`
`W = \int_B^A F dx ( - 1)`
`W = - \int_B^A F dx `
Therefore work done in bringing test charge `q_0` from infinity to point P at r distance.
`W = - \int_{\infty}^r F dx `
`W = - \int_{\infty}^r \frac{K q q_0}{x^2} dx ` (OB = x)
`W = - K q q_0 \int_{\infty}^r \frac{1}{x^2} dx `
`\frac{W}{q_0} = - K q \int_{\infty}^r x^{-2} dx `
`V = - K q [\frac{x^{-2 + 1}}{- 2 + 1}]_{\infty}^r` `(\because \frac{W}{q_0} = V)`
`V = - K q [\frac{x^{- 1}}{- 1}]_{\infty}^r`
`V = + K q [\frac{1}{x}]_{\infty}^r`
`V = K q [\frac{1}{r} - \frac{1}{\infty}]`
`V = K q [\frac{1}{r} - 0]`
`V = K q [\frac{1}{r}]`
`V = \frac{K q}{r}`
Thus, electric potential decreases with an increase in r.
The formula `V = \frac{K q}{r}` is used in calculating the electric potential due to the electric dipole at `r, \theta` point.
Short Answer Type Questions
Numerical Questions
NCERT Chapter 2 Physics class 12
- Electric Potential
- Potential due to a Point Charge
- Electric Potential due to Charged Conducting Sphere with Derivation
- Electric Potential Due to Charged Conducting Sphere
- Electric Potential Due to Charged Non-Conducting Sphere
- Electric Potential due to Dipole at any Point
- Equipotential Surfaces and Properties of Equipotential Surface
- Electric Potential Due to Electric Dipole
- Electric Potential Due to a Group of Charges and Relation between Electric Field and Potential
- Electric Potential Energy of a System of Two-Point Charges
- Define the Electrostatic Potential Energy of a System of Two and Three-Point Charges
- Work in Rotation of Electric Dipole in Electric Field
- Potential Energy of a Dipole in an External Field
- Electrostatics of Conductors
- Dielectrics and polarization
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