The problem involves calculating the torque on a current-carrying rectangular loop placed in a magnetic field. To solve this, we utilize the formula for torque \((\tau)\) on a current-carrying loop in a magnetic field, given by:
\(\tau = n \cdot I \cdot A \cdot B \cdot \sin(\theta)\)
where:
The dimensions of the loop are given: 20 cm and 10 cm. Convert these to meters to calculate the area:
\(A = 0.2 \, \text{m} \times 0.1 \, \text{m} = 0.02 \, \text{m}^2\)
The loop is in the Y-Z plane, and the magnetic field is along the positive Y-direction. Therefore, the angle \(\theta = 90^\circ\) since the normal to the Y-Z plane is along the X-axis, which is perpendicular to the Y-direction.
Substituting the values into the torque formula:
\(\tau = 1 \times 5 \, \text{A} \times 0.02 \, \text{m}^2 \times 2 \times 10^{-3} \, \text{T} \times \sin(90^\circ)\)
\(\tau = 2 \times 10^{-4} \, \text{N} \cdot \text{m}\)
Now, to determine the direction of the torque, we use the right-hand rule for the cross product \(\mathbf{A} \times \mathbf{B}\). The fingers point in the direction of the area vector (normal to the loop, along the X-axis), and when curled towards the magnetic field (Y-direction), the thumb points in the result direction, which is the torque direction.
Given the current's anticlockwise direction concerning the negative X-axis, the torque direction will be opposite to the direction of the conventional curl from Y to Z direction, i.e., along the negative Z-direction.
Therefore, the correct answer is \(2 \times 10^{-4} \, \text{N} \, \text{m}\) along negative Z-direction.
The magnetic moment \( \vec{M} \) is given by:
\[ \vec{M} = I \vec{A}. \]With \( I = 5 \, \text{A} \), \( A = 0.2 \times 0.1 = 0.02 \, \text{m}^2 \), and \( \vec{A} = 0.02 \, \hat{i} \), we get:
\[ \vec{M} = 5 \times 0.02 \, \hat{i} = 0.1 \, \hat{i}. \]The torque \( \vec{\tau} \) is given by:
\[ \vec{\tau} = \vec{M} \times \vec{B}. \]Substituting \( \vec{B} = 2 \times 10^{-3} \, \hat{j} \):
\[ \vec{\tau} = 0.1 \, \hat{i} \times 2 \times 10^{-3} \, \hat{j} = 2 \times 10^{-4} \, (-\hat{k}) = 2 \times 10^{-4} \, \text{Nm}. \]Therefore, the answer is:
\[ 2 \times 10^{-4} \, \text{Nm} \text{ along the negative Z-direction.} \]A square Lamina OABC of length 10 cm is pivoted at \( O \). Forces act at Lamina as shown in figure. If Lamina remains stationary, then the magnitude of \( F \) is: 
Let R = {(1, 2), (2, 3), (3, 3)}} be a relation defined on the set \( \{1, 2, 3, 4\} \). Then the minimum number of elements needed to be added in \( R \) so that \( R \) becomes an equivalence relation, is: