Yes thank you that's the sort of questions i am struggling with! 
So for Q12, the force acting on the wire PQ is given by F=BILsinθ (θ is the angle of the wire in relation to the field), and so in both cases the angle is 90°. As the coil rotates through 360° the current supplied is constant, the length PQ does not change, and the magnetic field is constant in the case of the parallel field, and may be considered uniform in the case of the radial field. So the answer should be C..
Love your answer for Q14, but the one for Q12 is just a tiny bit off - Let me help

For Q12, we remember that \(\tau=nBIA\cos{\theta}\), the torque is dependent on the angle of the coil with the field. What the
radial field does is eliminates this angle - As you hint at, it is considered to always be \(\theta=90^\circ\). So, the magnitude of the torque for the radial motor is constant. For the parallel field motor, it varies sinusoidally with the \(\cos{\theta}\) term. In both, we need the torque to swap magnitude every half turn.
The graph that matches is actually
B - The radial field has constant magnitude of torque (just swapping direction), and the parallel field has sinusoidal variation as required

As for your question on how to tackle graphs, Mate, unfortunately there aren't any shortcuts. You just have to know the content. Use process of elimination to knock out obviously incorrect answers to give yourself the best chances of a correct answer. But the fact you are struggling with these is normal - They are tough questions
