The work done in moving a charge \( q \) in an electric field is given by: \[ W = \int_{x_1}^{x_2} q E \, dx \] For a unit charge (\( q = 1 \)), this simplifies to: \[ W = \int_{x_1}^{x_2} E \, dx \] (i) Work Done from \( (5 m, 0) \) to \( (10 m, 0) \)
Since the electric field is along the \( x \)-axis, we compute: \[ W = \int_{5}^{10} (10x + 4) \, dx \] \[ W = \left[ 10 \frac{x^2}{2} + 4x \right]_{5}^{10} \] \[ W = \left( 5 \times 100 + 4 \times 10 \right) - \left( 5 \times 25 + 4 \times 5 \right) \] \[ W = (500 + 40) - (125 + 20) \] \[ W = 540 - 145 = 395 \text{ J} \] Thus, the work done is 395 J.
(ii) Work Done from \( (5 m, 0) \) to \( (5 m, 10 m) \) - Since the electric field is only along the \( x \)-direction (\( E_x \)), there is no electric field component in the \( y \)-direction.
- Work is only done when moving in the direction of the field. Since displacement in the \( x \)-direction is zero, the work done is: \[ W = 0 \] Thus, the work done is 0 J.
A point charge $ +q $ is placed at the origin. A second point charge $ +9q $ is placed at $ (d, 0, 0) $ in Cartesian coordinate system. The point in between them where the electric field vanishes is:
A small bob of mass 100 mg and charge +10 µC is connected to an insulating string of length 1 m. It is brought near to an infinitely long non-conducting sheet of charge density \( \sigma \) as shown in figure. If the string subtends an angle of 45° with the sheet at equilibrium, the charge density of sheet will be :
Consider two infinitely large plane parallel conducting plates as shown below. The plates are uniformly charged with a surface charge density \( +\sigma \) and \( -\sigma \). The force experienced by a point charge \( +q \) placed at the mid point between the plates will be:
The correct IUPAC name of \([ \text{Pt}(\text{NH}_3)_2\text{Cl}_2 ]^{2+} \) is: