I'll take belt drive over the over versions and here is why. First, belt drive tt's in general have high mass platters. That provides not just speed stability but also dampening; dampening not just external vibrations but also motor cogging. The mass of the platter provides inertia to help keep the speed constant. For example, my tt has a 14lbs (6.36kg) platter. A 1 gram change in stylus drag (assuming a drastic change in the record groove) generates 0.00155Nm of torque at the outer rim of the record. Assuming all else is constant except for this torque change, the platter is going to lose 0.29% of its speed in 1 second. Of course the motor is going to increase torque to compensate, but for this analysis you can see the impact of stylus drag on the platter. The deceleration is proportional to platter mass, so if your platter weighs 28lbs, then the speed loss would be half or 0.145%. Conversely, the stylus drag will have a proportionally larger impact on lighter flywheels. Motor speed control and belt compliance play a larger roll in speed stability than inertia, but I wanted to point out the value of higher mass platters. Now imagine a low mass platter directly coupled to a motor. Not saying it is impossible, but it is definitely an engineering challenge to smooth out the torque ripples from the motor and isolate the record from external vibrations.
- ...
- 361 posts total
- 361 posts total