(E) Magnetic field strength,$B = 3000 \; G = 3000 \times 10^{-4} \; T = 0.3 \; T$.
Length of the rectangular loop,$l = 10 \; cm = 0.1 \; m$.
Width of the rectangular loop,$b = 5 \; cm = 0.05 \; m$.
Area of the loop,$A = l \times b = 0.1 \times 0.05 = 50 \times 10^{-4} \; m^2$.
Current in the loop,$I = 12 \; A$.
The magnetic moment is $\vec{m} = I \vec{A}$. The torque is $\vec{\tau} = \vec{m} \times \vec{B}$.
In a uniform magnetic field,the net force on a current loop is always zero.
$(a)$ $\vec{A}$ is along the $x-$axis. $\vec{m} = I A \hat{i}$. $\vec{\tau} = (I A \hat{i}) \times (B \hat{k}) = -I A B \hat{j} = -1.8 \times 10^{-2} \hat{j} \; Nm$.
$(b)$ Similar to $(a)$,$\vec{\tau} = -1.8 \times 10^{-2} \hat{j} \; Nm$.
$(c)$ $\vec{A}$ is along the $y-$axis. $\vec{m} = I A \hat{j}$. $\vec{\tau} = (I A \hat{j}) \times (B \hat{k}) = I A B \hat{i} = 1.8 \times 10^{-2} \hat{i} \; Nm$.
$(d)$ The angle between $\vec{m}$ and $\vec{B}$ is $60^{\circ}$. $|\vec{\tau}| = m B \sin(60^{\circ}) = 1.8 \times 10^{-2} \times \frac{\sqrt{3}}{2} \approx 1.56 \times 10^{-2} \; Nm$.
$(e)$ $\vec{m}$ is along the $z-$axis. $\vec{m} = I A \hat{k}$. $\vec{\tau} = (I A \hat{k}) \times (B \hat{k}) = 0$. This is stable equilibrium as $\vec{m} \parallel \vec{B}$.
$(f)$ $\vec{m}$ is along the $-z-$axis. $\vec{\tau} = 0$. This is unstable equilibrium as $\vec{m}$ is anti-parallel to $\vec{B}$.