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For other uses, see Flywheel (disambiguation).
Trevithick's 1802 steam locomotive used a flywheel to even out the power of its single cylinder
G2 Flywheel Module, NASA
Flywheel movement
An industrial flywheel.

A flywheel is a rotating mechanical device that is used to store rotational energy. Flywheels have an inertia called the moment of inertia and thus resist changes in rotational speed. The amount of energy stored in a flywheel is proportional to the square of its rotational speed. Energy is transferred to a flywheel by the application of a torque to it, thereby increasing its rotational speed, and hence its stored energy. Conversely, a flywheel releases stored energy by applying torque to a mechanical load, thereby decreasing the flywheel's rotational speed.

Common uses of a flywheel include:

  • Providing continuous energy when the energy source is discontinuous. For example, flywheels are used in reciprocating engines because the energy source, torque from the engine, is intermittent.
  • Delivering energy at rates beyond the ability of a continuous energy source. This is achieved by collecting energy in the flywheel over time and then releasing the energy quickly, at rates that exceed the abilities of the energy source.
  • Controlling the orientation of a mechanical system. In such applications, the angular momentum of a flywheel is purposely transferred as a torque to the attaching mechanical system when energy is transferred to or from the flywheel, thereby causing the attaching system to rotate into some desired position.

Flywheels are typically made of steel and rotate on conventional bearings; these are generally limited to a revolution rate of a few thousand RPM.[1] Some modern flywheels are made of carbon fiber materials and employ magnetic bearings, enabling them to revolve at speeds up to 60,000 RPM.[2]

Carbon-composite flywheel batteries have recently been manufactured and are proving to be viable in real-world tests on mainstream cars. Additionally, their disposal is more eco-friendly.[3]


A Landini tractor with exposed flywheel.

Flywheels are often used to provide continuous energy in systems where the energy source is not continuous. In such cases, the flywheel stores energy when torque is applied by the energy source, and it releases stored energy when the energy source is not applying torque to it. For example, a flywheel is used to maintain constant angular velocity of the crankshaft in a reciprocating engine. In this case, the flywheel—which is mounted on the crankshaft—stores energy when torque is exerted on it by a firing piston, and it releases energy to the crankshaft when a piston is in the process of compressing a fresh charge of air and fuel. Other examples of this are friction motors, which use flywheel energy to power devices such as toy cars.

Modern automobile engine flywheel

A flywheel may also be used to supply intermittent pulses of energy at transfer rates that exceed the abilities of its energy source, or when such pulses would disrupt the energy supply (e.g., public electric network). This is achieved by accumulating stored energy in the flywheel over a period of time, at a rate that is compatible with the energy source, and then releasing that energy at a much higher rate over a relatively short time when it is needed. For example, flywheels are used in riveting machines to store energy from the motor and release it during the riveting operation.

The phenomenon of precession has to be considered when using flywheels in vehicles. 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, that is rigidly attached to the vehicle, would experience an torque applied to the body of the vehicle that would rotate with as the flywheel precesses. This would produce an alternating rolling and pitching of the vehicle body as it moved up the incline. The descent of the hill would produce the opposite effect and so it would zero out the pitching and rolling (roll momentum in response to a pitch change). Two counter-rotating flywheels may be needed to eliminate this effect. This effect is used in reaction wheels, a type of flywheel employed in satellites in which the flywheel is used to orient the satellite's instruments without the use of thruster rockets. Alternatively, the flywheel would be mounted in two yokes, with axes at mutual right angles, and so allow limited changes to the orientation of the vehicle body thereby eliminating precession.


The principle of the flywheel is found in the Neolithic spindle and the potter's wheel.[4]

The use of the flywheel as a general mechanical device to equalize 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. 1070–1125) who records applying the device in several of his machines.[4][5]

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 motion into rotary motion.


A flywheel with variable moment of inertia, conceived by Leonardo da Vinci.

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:

  • E_k=\frac{1}{2} I \omega^2


  • ω 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 when a given force is applied).
  • The moment of inertia for a solid cylinder is I = \frac{1}{2} mr^2,
  • for a thin-walled empty cylinder is I = m r^2,
  • and for a thick-walled empty cylinder is I = \frac{1}{2} m({r_\mathrm{external}}^2 + {r_\mathrm{internal}}^2) ,[6]

Where m denotes mass, and r denotes a radius.

When calculating with SI units, the units would be for mass, kilograms; for radius, meters; and for angular velocity, radians per second and the resulting energy 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 that develop within the rotor is a major consideration in the design of a flywheel energy storage system.

  •  \sigma_t = \rho r^2 \omega^2 \


  •  \sigma_t is the tensile stress on the rim of the cylinder
  •  \rho is the density of the cylinder
  •  r is the radius of the cylinder, and
  •  \omega is the angular velocity of the cylinder.

This formula can also be simplified using specific tensile strength and tangent velocity:

  •  \frac{\sigma_t}{\rho} = v^2


  •  \frac{\sigma_t}{\rho} is the specific tensile strength of the material
  •  v is the tangent velocity of the rim.

Material Selection[edit]

Small flywheels made of lead are found in children’s toys. Cast iron flywheels are used in old steam engines. Flywheels are used in cars to smooth power-transmission. Flywheels made from high-strength steel or composites have been proposed for use in vehicle power storage and braking systems. Flywheels are made from a breadth of materials, but what criteria is used to determine the best choice?

The efficiency of a flywheel is determined by the amount of energy it can store per unit weight. As the flywheel’s rotational speed or angular velocity is increased, the stored energy increases; however, the centrifugal stresses also increase. If the centrifugal stresses surpass the tensile strength of the material, the flywheel will fly apart. Thus, the tensile strengths is an upper limit to the amount of energy that a flywheel can store.

In this context, using lead for a flywheel in a child’s toy is not efficient; however, the flywheel velocity never approaches its burst velocity because the limit in this case is the pulling-power of the child. In other applications, such as an automobile, the flywheel operates at a specified angular velocity and is constrained by the space it must if in, so the goal is to maximize the stored energy per unit volume. The answer therefore depends on the application [7]

The table below contains calculated values for materials and comments one their viability for flywheel applications.

Material Specific tensile strength (\frac{kJ}{kg}) \ Comments
Ceramics 200-2000 (compression only) Brittle and weak in tension, therefore eliminate
Composites: CFRP 200-500 The best performance--a good choice
Composites: GFRP 100-400 Almost as good as CFRP and cheaper
Beryllium 300 The best metal, but expensive, difficult to work with, and toxic to machine
High strength steel 100-200 Cheaper than Mg and Ti alloys
High strength Al alloys 100-200 Cheaper than Mg and Ti alloys
High strength Mg alloys 100-200 About equal performance to steel and Al-alloys
Ti alloys 100-200 About equal performance to steel and Al-alloys
Lead alloys 3 Very low
Cast Iron 8-10 Very low


The table below shows calculated values for mass, radius, and angular velocity for storing 500 J. The carbon-fiber flywheel is by far the most efficient; however, it also has the largest radius. In applications (like in an automobile) where the volume is constrained, a carbon-fiber flywheel might not be the best option.

Material Energy Storage (J) Mass (kg) Radius (m) Angular velocity (rpm) Efficiency (J/kg)
Cast Iron 500 0.0166 1.039 1465 30121
Aluminum Alloy 500 0.0033 1.528 2406 151515
Maraging steel 500 0.0044 1.444 2218 113636
Composite: CFRP (40% epoxy) 500 0.001 1.964 3382 500000
Composite: GFRP (40% epoxy 500 0.0038 1.491 2323 131579


Table of energy storage traits[edit]

Flywheel purpose, type Geometric shape factor (k)
(unitless – varies with shape)
Angular velocity
Energy stored
Energy stored
Energy density (kWh/kg)
Small battery 0.5 100 60 20,000 9.8 2.7 0.027
Regenerative braking in trains 0.5 3000 50 8,000 33.0 9.1 0.003
Electric power backup[10] 0.5 600 50 30,000 92.0 26.0 0.043


For comparison, the energy density of petrol (gasoline) is 44.4 MJ/kg or 12.3 kWh/kg.

High-energy materials[edit]

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:

  • E_k \varpropto \frac{\sigma_t}{\rho}m

\frac{\sigma_t}{\rho} 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:

  • E_k \varpropto \sigma_tV


A rimmed flywheel has a rim, a hub, and spokes.[15] Calculation of the flywheel's moment of inertia can be more easily analysed by applying various simplifications. For example:

  • Assume the spokes, shaft and hub have zero moments of inertia, and the flywheel's moment of inertia is from the rim alone.
  • The lumped moments of inertia of spokes, hub and shaft may be estimated as a percentage of the flywheel's moment of inertia, with the majority from the rim, so that I_\mathrm{rim}=KI_\mathrm{flywheel}

For example, if the moments of inertia of hub, spokes and shaft are deemed negligible, and the rim's thickness is very small compared to its mean radius (R), the radius of rotation of the rim is equal to its mean radius and thus:

  • I_\mathrm{rim}=M_\mathrm{rim}R^2

See also[edit]


  1. ^ [1]; "Flywheels move from steam age technology to Formula 1"; Jon Stewart | 1 July 2012, retrieved 2012-07-03
  2. ^ [2], "Breakthrough in Ricardo Kinergy ‘second generation’ high-speed flywheel technology"; Press release date: 22 August 2011. retrieved 2012-07-03
  3. ^
  4. ^ a b Lynn White, Jr., "Theophilus Redivivus", Technology and Culture, Vol. 5, No. 2. (Spring, 1964), Review, pp. 224–233 (233)
  5. ^ Lynn White, Jr., "Medieval Engineering and the Sociology of Knowledge", The Pacific Historical Review, Vol. 44, No. 1. (Feb., 1975), pp. 1–21 (6)
  6. ^ [3] (page 10, accessed 1 Dec 2011, Moment of inertia tutorial
  7. ^ Ashby, Michael (2011). Materials Selection in Mechanical Design (4th ed.). Burlington, MA: Butterworth-Heinemann. pp. 142–146. ISBN 978-0-08-095223-9. 
  8. ^ Totten, George E.; Xie, Lin; Funatani, Kiyoshi (2004). Handbook of Mechanical Alloy Design. New York: Marcel Dekker. ISBN 0-8247-4308-3. 
  9. ^ Kumar, Mouleeswaran Senthil; Kumar, Yogesh (2012). "Optimization of Flywheel Materials Using Genetic Algorithm" (PDF). Acta technica Corviniensis-Bulletin of Engineering. Retrieved 1 November 2015. 
  10. ^
  11. ^ "Flywheel Energy Calculator". 2004-01-07. Retrieved 2010-11-30. 
  12. ^ "energy buffers". Retrieved 2010-11-30. 
  13. ^ "Message from the Chair | Department of Physics | University of Prince Edward Island". Retrieved 2010-11-30. 
  14. ^ "Density of Steel". 1998-01-20. Retrieved 2010-11-30. 
  15. ^ Flywheel Rotor And Containment Technology Development, FY83. Livermore, Calif: Lawrence Livermore National Laboratory , 1983. pp. 1–2

External links[edit]