The torque acting on a current-carrying coil in a magnetic field is given by:
\[
\tau = nIBA \sin \theta
\]
Where:
- \( n = 30 \) is the number of turns,
- \( I = 6 \, \text{A} \) is the current,
- \( B = 1.0 \, \text{T} \) is the magnetic field strength,
- \( A = \pi r^2 = \pi (0.08)^2 \, \text{m}^2 \) is the area of the coil,
- \( \theta = 30^\circ \) is the angle between the magnetic field and the normal to the coil.
Substituting the values:
\[
\tau = 30 \times 6 \times \pi \times (0.08)^2 \times \sin 30^\circ = 1.8 \, \text{Nm}
\]
Thus, the counter torque required is \( \boxed{1.8 \, \text{Nm}} \).