:biggrinbounce2: You can not have one with out the other. However you can lean towards one over the other. Personal feeling here is that when you lean towards the torque end of the equation you will get a much wider ability to tune your bar length, raker hight, chain style and sprocket size. With a saw built towards the RPM end of the equation everything else has to be tailored to the RPM of the saw and is a lot less utilitarian.
I'll make a modification to your statement.
In an internal combustion engine, neither horsepower nor torque cannot exist without the other.
An example:
Ever spin a torque wrench? Then you know you can apply torque (twisting force) to a bolt and not move it. With the physics equation WRW quoted, we would generate zero horsepower no matter how much torque we applied as long as the bolt
does not turn.
(Torque x bolt rpm) / 5,252 = Horsepower
so, (100 ft/lbs x 0)/5252 = Horsepower
then, 0=0 but we still applied torque - we just didn't make any horsepower.
If we plug in zero for torque
(0 ft/lbs x 0 rpm)/5252 = horsepower
0=0 it's a multiplication by zero.
There's no way we can make horsepower with the above equation because we can't accelerate from zero rpm. We can't apply a "twisting force" if torque = 0.
Now we know that horsepower is dependent on torque, but torque is not dependent on horsepower.
Sometimes it is said that the characteristics of the torque curve define how high the horsepower curve goes. Obviously, if the torque peak is low in the rpm range, top rpm will be limited but if we can move the torque curve up the rpm scale, we can generate more horsepower simply because we have more powerstrokes per minute.
So let's look at an example of a piston driven engine such as a chainsaw. The piston goes up and down. So, when ignition happens in a chainsaw, the piston and rod exhibit a torque on the crankshaft throw and the piston accelerates downward. Past mid stroke, it begins to decelerate, then the piston stops, reverses direction and accelerates to TDC. The torque applied to the crankshaft in the powerstroke establishes momentum in the crankshaft that carries the piston back to TDC.
We can now imagine that the rpm's of the saw can reach a point where the torque is unable to accelerate the piston any faster in the powerstroke. Peak rpm. But if we had a little more torque, we could spin more rpms thus creating more horsepower. Simple, eh?
It's the shape of the torque curve that defines how many rpm's your saw is going to turn and how much horsepower it's going to make.