The friction of the belt and pulley is what you want. That's the load you are putting on the mechanism. The friction from the slippage will cause heat thus dissipating power from the turbine.
You could use a greased belt but then you'd need a bunch of force on the spring scales to get friction or a dry sticky strap of leather in which case you'd need less force on the scales. In either case you subtract the force on scale B from scale A leaving you zero... until you start turning the shaft.
Let's say you have the shaft spinning in a stiff breeze at 100rpm with the belt slack. You start tightening up the belt until your rpms fall to a reasonably steady 50 rpm. You read the scales and find that one of them reads 8 pounds and the other reads 30 pounds. 30-8=22lbs. Multiply this by the radius of the wheel in feet and you have torque in pound feet.
Multiply the torque by the rpm and divide by 5252 to get Horse Power and divide HP by 746 to get watts.
Now try slacking up the belt some to drop the torque but the rpms increase. If the torque drops by 10 % but the rpms increase by 30%, then your total power in watts has increased by 17%.
On the other hand if your torque drops by 10% but your rpms only increase by 5% then your total power has dropped by 5.5% Any given turbine will have an optimum torque and rpm for a given windspeed for maximum total power out. This where Tip Speed Ratio comes in.
This is the heart of matching the alternator (and the load) to the turbine. Part of the trick is trying to design things to be as max as possible over the full range of possible windspeeds and (usually) preferably in the most common windspeeds
Hope this helps. I'm sure someone will jump in if I got this seriously wrong.