TO begin with, lets define horsepower and 'Torque'. Torque produced at the crank is called a 'moment' since it rotates on an axis. An imaginary line across the 2 ends of a crank is the axis.
Torque in this case is Force X Perpendicular distance.
Long stroke engines have more perpendicular distance and a relatively smaller bore.
Force or combustion is what drives the piston down. So Torque characteristics can vary on identical engines with different piston face designs, number of valves and compression ratio and so on.
However, it's not necessarily true that only long stroke engines produce more torque. You could have a short-stroke engine producing more torque than a long-stroke or a square engine. But it's always true that the torque characteristics would greatly vary between the 2 aforementioned engines -- the long stroke would typically produce more torque at lower rpms.
There is more friction in long stroke engines as pistons need to travel a greater distance per stroke. Also, smaller or restricted head-design would limit the speed of a long stroke engine as compared to a short-stroke engine. It is mostly true that a short-stroke engine will allow higher engine speeds as compared to long stroke engines.
Now talking about James Watt's definition of horsepower, 1 HP is equivalent to vertically lifting 33 pounds of mass upto 100 feet in one minute.
You can imagine a 1 HP elevator 'A' that travels hundred feet up and can only carry 33 pounds and takes 1 minute to reach a hundred feet.
Another elevator 'B' travels 1 feet up and can carry 3300 pounds and takes a minute to reach 1 foot from where it started originally. Both elevators produce exacctly 1 HP.
1 HP = no of feet travelled by the elevator vertically X Mass = 33000 Foot Pounds.
Lets take rotational forces into consideration.
Eg. 1 :
1 HP = circumference in feet X Mass
If the circumference of a flywheel is 10 feet and 100 pounds of force is applied to rotate the flywheel, the flywheel moves at :
[(1 HP / Circumference) / Force]
= (33000 / 10) /100 = 33 RPM
Eg 2 :
If the circumference of the flywheel is 65 feet and 100 pounds of force is applied to rotate the flywheel, the flywheel moves at:
[(1 HP / Circumference) / Force]
= (33000 / 65) /100 = 5.076 RPM
Yet both produce the same Horsepower at different RPMS !
We all know that circumference = pi*d = 2*pi*r
Circumference is nothing but the distance travelled by the flywheel to complete a revolution.
Horsepower = (Torque * RPM) / (33,000 / 2* pi)
= Torque X RPM / 5252
The last equation just shows us that RPMs have a lot to do with Horsepower too. There is such strong correlation with horsepower , torque and RPM.
To conclude : It doesn't matter what the displacement of the engine is, what matters is the way the engine produces power, the way the power is delivered to the wheels (taking frictional losses into consideration) and the number of gears + gearing rations for the vehicle.
For vehicles with a really narrow power-band (eg: Volvo buses) it makes sense to have 6-7 gears. |