## What is Electric Field Intensity?

The space around an electric charge in which its influence can be felt is known as the **electric field**. TheÂ **electric field Intensity**Â at a point is the force experienced by a unit positive charge placed at that point.

- Electric Field Intensity is a vector quantity.
- It is denoted by ‘E’.
- Formula: Electric Field = F/q.
- Unit of E is NC
^{-1}or Vm^{-1}.

The electric field intensity due to a positive charge is always directed away from the charge and the intensity due to a negative charge is always directed towards the charge.

### Table of Content:

Due to a point charge q, the intensity of the electric field at a point d units away from it is given by the expression:

Electric Field Intensity (E) = q/[4Ï€Îµd^{2}] NC^{-1}

The intensity of the electric field at any point due to a number of charges is equal to the vector sum of the intensities produced by the separate charges.

## Force Experienced by a Charge in Electric Field

The force experienced by a charge in an electric field is given by, \(\vec{F}=Q\vec{E}\). where E is the electric field intensity.

### Special Cases:

- If
**Q is a positive charge**, the force \(\vec{F}\) acts in the direction of \(\vec{E}\) . Acceleration a = F/m = QE/m. - If
**Q is a negative charge**, the force acts in a direction opposite to \(\vec{E}\). Acceleration a = F/m = QE/m

A charge in an electric field experiences a force whether it is at rest or moving. The electric force is independent of the mass and velocity of the charged particle, it depends upon the charge.

#### â‡’ Also Read:

## Motion of Charged Particle in Electric Field

If a charged particle of charge Q is placed in an electric field of strength E, the force experienced by the charged particle = EQ.

- The acceleration of the charged particle in the electric field, a = EQ/m.
- The velocity of the charged particle after time t is = (EQ/m)t if the initial velocity is zero.
- The distance travelled by the charged particle is S = 1/2Â Ã— at
^{2}= 1/2(EQ/m) Ã— t^{2}if the initial velocity is zero.

### The Trajectory of Particle in Electric Field

When a charged particle is projected into a uniform electric field with some velocity perpendicular to the field, the path traced by it is a parabola. The trajectory of a charged particle projected in a different direction from the direction of a uniform electric field is a parabola.

- When a charged particle of mass m and charge Q remains suspended in a vertical electric field then mg = EQ.
- When a charged particle of mass m and charge Q remains suspended in an electric field and the number of fundamental charges on the charged particle is n then,Â
**mg = E(ne),**thusÂ n = mg/Ee.

### Pendulum Oscillating in a Uniform Electric Field

The bob of a simple pendulum is given +ve charge and it is made to oscillate in vertically upward electric field, then the time period of oscillation is

Time Period (T) = 2Ï€ Ã— âˆš[l/(g –Â EQ/m)]

In the above case, if the bob is given a -ve charge then the time period is given by;

Time Period (T) = 2Ï€ Ã— âˆš[l/(g + EQ/m)]

### Projectile Motion in an Electric Field

A charged particle is projected with an initial velocity u andÂ charge Q making an angle to the horizontal in an electric field directed vertically upward then,

1. Time of flight = 2u sin Î¸/[g Â± EQ/m]

2. Maximum height = u^{2} sin^{2} Î¸/[g Â± EQ/m]

3. Range = u^{2} sin 2Î¸/[g Â± EQ/m]

## Properties of Charged Particle in Electric Field

**1.**Â The density of the electric field inside a charged hollow conducting sphere is zero.

**2.Â **A sphere is given a charge of â€˜Qâ€™ and is suspended in a horizontal electric field. The angle made by the string with the vertical is, Î¸ = Tan^{-1}Â (EQ/mg).

**3.Â **The tension in the string isÂ âˆš(EQ^{2}Â + mg^{2}).

**4.** A bob carrying a +ve charge is suspended by a silk thread in a vertically upward electric field, then the tension in the string is; T = mg – EQ.

**5.** If the bob carries -ve charge, the tension in the string is; T = mg + EQ.

### Force Experienced by Electron and Proton

A proton and an electron in the same electric field experience forces of the same magnitude but in opposite directions. Force on the proton is accelerating force whereas force on the electron is retarding force. If the proton and electron are initially moving in the direction of the electric field.

Acceleration of proton/Retardation of electron = mass of an electron/mass of a proton.

## Solved Example

**Question:**Â A rigid insulated wireframe in the form of a right-angled triangle ABC, is set in a vertical plane as shown. Two beads of equal masses m and carrying charges q1 and q2 are connected by a cord of length L and can slide without friction on the wires. Considering the case when the beads are stationary, determine,

- The angle Î± (âˆ APQ),
- The tension in the cord,
- The normal reactions on the beads.
- If the cords are now cut, what are the values of the charges for which the beads continue to remain stationary?

**Solution:**

**1.** The forces acting on each bead are,

- mg (downward)
- Tension
- Electric force
- Normal Reactions.

The directions of the forces are shown in the figure:

Equating the forces along and perpendicular to AB and AC, for equilibrium of the beads;

T cos Î± = F cos Î± + mg sin 30^{0}Â . . . . (1)

F sinÂ Î± + N1 = mg cos 30^{0}Â + T sinÂ Î± . . . . . (2)

T sinÂ Î± = F sinÂ Î± + mg cos 30^{0Â }. . . . . . (3)

N2 + F cosÂ Î± = T cosÂ Î± + mg cos 60^{0}Â . . . . . (4)

From equation (1) and (3);

(T – F) cosÂ Î± = mg sin 30^{0}

and (T – F) sinÂ Î± = mg cos 30^{0}

Dividing, cotÂ Î± = tan 30^{0}Â = cot 60^{0}

Therefore,Â Î± = 60^{0}.

**â‡’ Check:Â **Equipotential surfaces and their properties

**2.** Substituting the value of Î± in (1) and noting that

F = \(\frac{1}{4\pi {{\varepsilon }_{0}}}\;\;\frac{{{q}_{1}}{{q}_{2}}}{{{\ell }^{2}}}\)

T cos 60Âº= \(\frac{1}{4\pi {{\varepsilon }_{0}}}\;\;\frac{{{q}_{1}}{{q}_{2}}}{{{\ell }^{2}}}\) cos 60Âº + mg sin 60Âº

or T = \(\frac{1}{4\pi {{\varepsilon }_{0}}}\;\;\frac{{{q}_{1}}{{q}_{2}}}{{{\ell }^{2}}} + mg\).

**3.Â **T – F =\(\frac{mg\,\,\sin 30{}^\text{o}}{\cos 60{}^\text{o}}\) = mg

From (2), N1 = mg cos 30Âº + (T – F) sin 60Âº

â‡’ N1 = mg \(\frac{\sqrt{3}}{2} + mg . \frac{\sqrt{3}}{2}= \sqrt{3} mg\)

From (4), N2 = (T â€“ F) cos 60^{0}Â Â± mg cos 60^{0}

= mg Ã— 1/2 + mg Ã— 1/2 = mg.

**4.** When the cord is cut, T = 0, then from (1)

0 = F cos 60^{0}Â + mg sin 30^{0}

or F + mg = 0

This result is on the assumption that q1 and q2 are of the same sign, so it was taken that there was a force of repulsion.

Since mg is fixed in direction, its sign cannot be reversed but the sign of F can be reversed because if q1 and q2 are of opposite sign, F will change its sign from + to -.

Let q1 and q2 be of the opposite sign then,

-F + mg = 0 is the condition for equilibrium.

or \(\frac{1}{4\pi {{\varepsilon }_{0}}}\;\;\frac{{{q}_{1}}{{q}_{2}}}{{{\ell }^{2}}}\) = mg

or q1q2 = \(4\pi\varepsilon _0mg\lambda^{2}\)