To calculate the torque on a dipole, always ensure the units of electric field, charge, and distance are consistent. Convert non-SI units like dyne/C to N/C before substituting into the formula.
The torque acting on an electric dipole in a uniform electric field is given by:
\[ \tau = pE \sin \theta, \]where:
Step 1: Calculate the dipole moment (\( p \)).
The dipole moment is:
\[
p = q \cdot d = (0.01) \cdot (0.4 \times 10^{-3}) = 4 \times 10^{-6} \, \text{Cm}.
\]
Step 2: Substitute values into the torque formula.
The electric field is given in dyne/C. Convert it to SI units:
\[
1 \, \text{dyne/C} = 10^{-5} \, \text{N/C}, \quad E = 10 \times 10^{-5} = 10^{-4} \, \text{N/C}.
\]
Now substitute the values:
\[
\tau = (4 \times 10^{-6}) \cdot (10^{-4}) \cdot \sin 30^\circ.
\]
Step 3: Simplify the expression.
\[
\sin 30^\circ = 0.5,
\]
so:
\[
\tau = (4 \times 10^{-6}) \cdot (10^{-4}) \cdot 0.5 = 2 \times 10^{-10} \, \text{Nm}.
\]
An infinite sheet of uniform charge \( \rho_s = 10\, {C/m}^2 \) is placed on the \( z = 0 \) plane. The medium surrounding the sheet has a relative permittivity of 10 . The electric flux density, in C/m\(^2\), at a point \( P(0, 0, 5) \), is: Note: \( \hat{a}, \hat{b}, \hat{c} \) are unit vectors along the \( x, y, z \) directions, respectively.
A metallic ring is uniformly charged as shown in the figure. AC and BD are two mutually perpendicular diameters. Electric field due to arc AB to O is ‘E’ magnitude. What would be the magnitude of electric field at ‘O’ due to arc ABC?
Let the focal chord PQ of the parabola $ y^2 = 4x $ make an angle of $ 60^\circ $ with the positive x-axis, where P lies in the first quadrant. If the circle, whose one diameter is PS, $ S $ being the focus of the parabola, touches the y-axis at the point $ (0, \alpha) $, then $ 5\alpha^2 $ is equal to:
If the system of equations: $$ \begin{aligned} 3x + y + \beta z &= 3 \\2x + \alpha y + z &= 2 \\x + 2y + z &= 4 \end{aligned} $$ has infinitely many solutions, then the value of \( 22\beta - 9\alpha \) is:
Let $ A $ be the set of all functions $ f: \mathbb{Z} \to \mathbb{Z} $ and $ R $ be a relation on $ A $ such that $$ R = \{ (f, g) : f(0) = g(1) \text{ and } f(1) = g(0) \} $$ Then $ R $ is:
For $ \alpha, \beta, \gamma \in \mathbb{R} $, if $$ \lim_{x \to 0} \frac{x^2 \sin \alpha x + (\gamma - 1)e^{x^2} - 3}{\sin 2x - \beta x} = 3, $$ then $ \beta + \gamma - \alpha $ is equal to: