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Flywheel

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Flywheel

Flywheel from stationary engine. Note the castellated rim which was used to rotate the engine to the correct starting position by means of a lever

1898 illustration of a White and Middleton stationary engine; note the large twin flywheels

A Landini tractor with massive flywheel

1928 Lanz Bulldog showing the flywheels and a hot bulb engine

Zaschka helicopter with flywheels, Berlin Tempelhof Airport, 1930

Spoked flywheel A flywheel is a mechanical device with a 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 an intermittent load, such as a piston pump, is placed on it. Flywheels can be used to produce very high power pulses for 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 and power plants.

History
The principle of the flywheel is found in the Neolithic spindle and the potter's wheel.[1] The Andalusian agronomist Ibn Bassal (fl 10381075), in his Kitab al-Filaha, describes the flywheel effect employed in a water wheel machine, the saqiya.[2] The flywheel as a general mechanical device for equalizing the speed of rotation is, according to the American medievalist Lynn White, recorded in the De diversibus artibus (On various arts) of the German artisan Theophilus Presbyter (ca. 10701125) who records applying the device in several of his machines.[1][3] 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.

Physics
A flywheel is a spinning wheel or disc with a fixed axle so that rotation is only about one axis. Energy is stored in the rotor as kinetic energy, or more specifically, rotational energy:

Where:

is the angular velocity, and I is the moment of inertia of the mass about the center of rotation. The moment of inertia is the measure of resistance to torque applied on a spinning object (i.e. the higher the moment of inertia, the slower it will spin after being applied a given force).

The moment of inertia for a solid-cylinder is

for a thin-walled empty cylinder is and for a thick-walled empty cylinder is

, ,

Where m denotes mass, and r denotes a radius. When calculating with SI units, the standards would be for mass, kilograms; for radius, meters; and for angular velocity, radians per second. The resulting answer would be in joules. 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.

Where:

t is the tensile stress on the rim of the cylinder is the density of the cylinder r is the radius of the cylinder, and is the angular velocity of the cylinder.

Examples of energy stored


object bicycle wheel at 20 km/h bicycle wheel, double speed (40 km/h) bicycle wheel, double mass (20 km/h) Millstone grinding wheel wheel on train @ 60 km/h k (varies mass with shape) 1 1 1 1/2 1 kg 1 kg 2 kg diameter 700 mm 700 mm 700 mm angular velocity 150 rpm 300 rpm 150 rpm 200 rpm energy energy stored stored, J 15 J 60 J 30 J 1.68 kJ 4 103 Wh 16 103 Wh 8 103 Wh 0.47 Wh

245 kg 500 mm

1/2

942 kg 1 m

318 rpm

65 kJ

18 Wh

[1] giant dump truck wheel 1/2 @ 30 km/h (18 mph) small flywheel battery 1/2 [2] regenerative braking flywheel for trains 1/2 [3] electrical power backup flywheel [4]

1000 kg 2 m 100 kg 600 mm

79 rpm 20000 rpm

17 kJ 9.8 MJ

4.8 Wh 2.7 kWh

3000 kg 500 mm

8000 rpm

33 MJ

9.1 kWh

1/2

600 kg 500 mm

30000 rpm

92 MJ

26 kWh

the planet Earth 2/5 [5], Rotational energy


[5][6][7][8]

5.97 ~1 per day 2.6 1029 72 YWh ( 1024 12,725 km 27 10 g (696 rpm[4]) J Wh)

High-energy materials
For a given flywheel design, the kinetic energy is proportional to the ratio of the hoop stress to the material density and to the mass:

could be called the specific tensile strength. The flywheel material with the highest specific tensile strength will yield the highest energy storage per unit mass. This is one reason why carbon fiber is a material of interest. For a given design the stored energy is proportional to the hoop stress and the volume:

Applications
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. In a 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. Flywheels are used in punching machines and riveting machines, where they store energy from the motor and release it during the operation cycle (punching and riveting). For internal combustion engine applications, the flywheel is a heavy wheel mounted on the crankshaft. The main function of a flywheel is to maintain a constant angular velocity of the crankshaft.

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