The correct option is: (A):
\(\vec{p_1} = q \times 4 \times 10^{-3} \hat{j}\)
The potential \(V_0\) is given by:
\(V_0 = \frac{K \vec{p_1} \cdot \vec{r_1}}{|\vec{r_1}|^3}\)
Substituting the known values:
\(V_0 = \frac{9 \times 10^9 \times q \times [4 \times 10^{-3} \hat{j}] \cdot (0.1 \hat{i} + 0.1 \hat{j})}{\left(\sqrt{(0.1)^2 + (0.1)^2}\right)^3}\)
Simplifying the dot product:
\(V_0 = \frac{9 \times 10^9 \times q \times [0.4 \times 10^{-3}]}{(0.1)^2 \times 2 \sqrt{2}}\)
Now, +q and -q are moved to the points (-1,2) mm and (1,-2) mm, respectively. The new position vector is:
\(\vec{p} = q[-2 \hat{i} + 4 \hat{j}] \times 10^{-3}\)
The position vector \(\vec{r_1}\) remains:
\(\vec{r_1} = 0.1 \hat{i} + 0.1 \hat{j}\)
The new potential \(V\) is calculated as:
\(V = \frac{9 \times 10^9 (\vec{p}, \vec{r_1})}{|\vec{r_1}|^3}\)
Substituting the values:
\(V = \frac{9 \times 10^9 \times q \times [0.4 \times 10^{-3}]}{\left(\sqrt{(0.1)^2 + (0.1)^2}\right)^3}\)
Simplifying:
\(V = \frac{V_0}{2}\)
Thus, the new potential \(V\) is half of the original potential \(V_0\), confirming the relationship between the initial and final potentials.
The unit of $ \sqrt{\frac{2I}{\epsilon_0 c}} $ is: (Where $ I $ is the intensity of an electromagnetic wave, and $ c $ is the speed of light)
The dimension of $ \sqrt{\frac{\mu_0}{\epsilon_0}} $ is equal to that of: (Where $ \mu_0 $ is the vacuum permeability and $ \epsilon_0 $ is the vacuum permittivity)
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
A temperature difference can generate e.m.f. in some materials. Let $ S $ be the e.m.f. produced per unit temperature difference between the ends of a wire, $ \sigma $ the electrical conductivity and $ \kappa $ the thermal conductivity of the material of the wire. Taking $ M, L, T, I $ and $ K $ as dimensions of mass, length, time, current and temperature, respectively, the dimensional formula of the quantity $ Z = \frac{S^2 \sigma}{\kappa} $ is:
The waves that are produced when an electric field comes into contact with a magnetic field are known as Electromagnetic Waves or EM waves. The constitution of an oscillating magnetic field and electric fields gives rise to electromagnetic waves.
Electromagnetic waves can be grouped according to the direction of disturbance in them and according to the range of their frequency. Recall that a wave transfers energy from one point to another point in space. That means there are two things going on: the disturbance that defines a wave, and the propagation of wave. In this context the waves are grouped into the following two categories: