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If E(a) be the electric field strength o...

If `E_(a)` be the electric field strength of a short dipole at a point on its axial line and `E_(e)` that on the equatorial line at the same distance, then

A

`E_(e)=2E_(a)`

B

`E_(a)= 2E_(e)`

C

`E_(a)=E_(e )`

D

None of the above

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The correct Answer is:
To find the relationship between the electric field strengths \( E_a \) (on the axial line) and \( E_e \) (on the equatorial line) of a short dipole at the same distance, we can follow these steps: ### Step 1: Understand the Electric Field Formulas For a short dipole, the electric field strength at a point on the axial line is given by: \[ E_a = \frac{2kp}{r^3} \] where \( k \) is the Coulomb's constant, \( p \) is the dipole moment, and \( r \) is the distance from the dipole center to the point. For the electric field strength at a point on the equatorial line, the formula is: \[ E_e = \frac{kp}{r^3} \] ### Step 2: Set Up the Ratio of Electric Fields Since we are given that both fields are calculated at the same distance \( r \), we can set up the ratio of \( E_e \) to \( E_a \): \[ \frac{E_e}{E_a} = \frac{\frac{kp}{r^3}}{\frac{2kp}{r^3}} \] ### Step 3: Simplify the Ratio When we simplify the ratio, we notice that \( k \) and \( r^3 \) cancel out: \[ \frac{E_e}{E_a} = \frac{1}{2} \] ### Step 4: Rearranging the Equation From the ratio, we can rearrange it to express \( E_a \) in terms of \( E_e \): \[ E_a = 2E_e \] ### Conclusion Thus, the relationship between the electric field strengths at the axial and equatorial lines of a short dipole is: \[ E_a = 2E_e \]

To find the relationship between the electric field strengths \( E_a \) (on the axial line) and \( E_e \) (on the equatorial line) of a short dipole at the same distance, we can follow these steps: ### Step 1: Understand the Electric Field Formulas For a short dipole, the electric field strength at a point on the axial line is given by: \[ E_a = \frac{2kp}{r^3} \] where \( k \) is the Coulomb's constant, \( p \) is the dipole moment, and \( r \) is the distance from the dipole center to the point. ...
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