A flywheel is a mechanical device with significant moment of inertia used as a storage device for rotational energy. Flywheels resist changes in their rotational speed, which helps steady the rotation of the shaft when a fluctuating torque is exerted on it by its power source such as a piston-based (reciprocating) engine, or when the load placed on it is intermittent (such as a piston pump). Flywheels can be used to produce very high power pulses as needed for some experiments, where drawing the power from the public network would produce unacceptable spikes. A small motor can accelerate the flywheel between the pulses. Recently, flywheels have become the subject of extensive research as power storage devices for uses in vehicles; see flywheel energy storage.
where m denotes mass, and r denotes a radius. More information can be found at list of moments of inertia
The amount of energy that can safely be stored in the rotor depends on the point at which the rotor will warp or shatter. The hoop stress on the rotor is a major consideration in the design of a flywheel energy storage system.
You can use those equations to do 'back of the napkin' calculations and find the rotational energy stored in various flywheels. I = kmr², and k is from List of moments of inertia
|object||k (varies w shape)||mass||diameter||angular velocity||energy stored, J||energy stored, kWh|
|bicycle wheel||1||1 kg||700 mm||150 rpm||15 J||0.0000004 kWh|
|bicycle wheel, double speed||1||1 kg||700 mm||300 rpm||60 J||0.0000016 kWh|
|bicycle wheel, double mass||1||2 kg||700 mm||150 rpm||30 J||0.0000008 kWh|
|Flintstones concrete car wheel||1/2||245 kg||500 mm||200 rpm||1680 J||0.00047 kWh|
|wheel on train @ 60km/h||1/2||942 kg||1 m||318 rpm||65,000 J||0.018 kWh|
|giant dump truck wheel @ 18mph||1/2||1000 kg||2 m||79 rpm||17,000 J||0.0048 kWh|
|small flywheel battery||1/2||100 kg||600 mm||20000 rpm||9.8 MJ||2.7 kWh|
|regenerative braking flywheel for trains||1/2||3000 kg||500 mm||8000 rpm||33 MJ||9.1 kWh|
|electrical power backup flywheel||1/2||600 kg||500 mm||30000 rpm||92 MJ||26 kWh|
|the planet earth , Rotational_energy||2/5||5.97e24 kg||12725 km||1 per day||2.5e29 J||7e22 kWh|
See , , , , and Rotational_energy
For a given flywheel design, it can be derived from the equations above that the kinetic energy is proportional to the ratio of the hoop stress to the material density.
In application of flywheels in vehicles, the phenomenon of precession has to be considered. A rotating flywheel responds to any momentum that tends to change the direction of its axis of rotation by a resulting precession rotation. A vehicle with a vertical-axis flywheel would experience a lateral momentum when passing the top of a hill or the bottom of a valley (roll momentum in response to a pitch change). Two counter-rotating flywheels may be needed to eliminate this effect.
The flywheel has been used since ancient times, the most common traditional example being the potter's wheel. In the Industrial Revolution, James Watt contributed to the development of the flywheel in the steam engine, and his contemporary James Pickard used a flywheel combined with a crank to transform reciprocating into rotary motion.
In a more modern application, a momentum wheel is a type of flywheel useful in satellite pointing operations, in which the flywheels are used to point the satellite's instruments in the correct directions without the use of thruster rockets.
The flywheel as a general mechanical device for equalizing the speed of rotation is first described in the Kitab al-Filaha of the Andalusian engineer Ibn Bassal (fl. 1038-1075), who applies the device in a chain pump (saqiya) and noria.
According to the American medievalist Lynn Townsend White, Jr., such a flywheel is also recorded in the De diversibus artibus (On various arts) of the German artisan Theophilus Presbyter (ca. 1070-1125), who records applying the device in several of his machines.