# Difference between revisions of "Inertia"

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[[Image:Arc_circle.png|right|thumb|250px|Basic circle geometry]] | [[Image:Arc_circle.png|right|thumb|250px|Basic circle geometry]] | ||

− | Below is a derivation of rotational inertia from first principles, starting from the basics of circle geometry | + | Below is a basic derivation of power system rotational inertia from first principles, starting from the basics of circle geometry and ending at the definition of moment of inertia (and it's relationship to kinetic energy). |

The length of a circle arc is given by: | The length of a circle arc is given by: | ||

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:: <math>n</math> is the speed in [https://en.wikipedia.org/wiki/Revolutions_per_minute revolutions per minute] (rpm) | :: <math>n</math> is the speed in [https://en.wikipedia.org/wiki/Revolutions_per_minute revolutions per minute] (rpm) | ||

− | + | The kinetic energy of a circular rotating mass can be derived from the classical Newtonian expression for the [https://en.wikipedia.org/wiki/Kinetic_energy#Kinetic_energy_of_rigid_bodies kinetic energy of rigid bodies]: | |

: <math> KE = \frac{1}{2} mv^{2} = \frac{1}{2} m(\omega r)^{2}</math> | : <math> KE = \frac{1}{2} mv^{2} = \frac{1}{2} m(\omega r)^{2}</math> | ||

where <math>KE</math> is the rotational kinetic energy (Joules or kg.m<sup>2</sup>/s<sup>2</sup> or MW.s, all of which are equivalent) | where <math>KE</math> is the rotational kinetic energy (Joules or kg.m<sup>2</sup>/s<sup>2</sup> or MW.s, all of which are equivalent) | ||

− | :: <math>m</math> is the mass of the rotating | + | :: <math>m</math> is the mass of the rotating body (kg) |

− | Alternatively, rotational kinetic energy can be expressed as: | + | Alternatively, [https://en.wikipedia.org/wiki/Kinetic_energy#Rotating_bodies rotational kinetic energy] can be expressed as: |

: <math> KE = \frac{1}{2} I\omega^{2} </math> | : <math> KE = \frac{1}{2} I\omega^{2} </math> | ||

− | where <math>I = mr^{2}</math> is called the '''moment of inertia''' (kg.m<sup>2</sup>) | + | where <math>I = mr^{2}</math> is called the '''[https://en.wikipedia.org/wiki/Moment_of_inertia moment of inertia]''' (kg.m<sup>2</sup>) |

[[Category:Fundamentals]] | [[Category:Fundamentals]] |

## Revision as of 04:56, 24 August 2018

In power systems engineering, "inertia" is a concept that typically refers to rotational inertia or rotational kinetic energy. For synchronous systems that run at some nominal frequency (i.e. 50Hz or 60Hz), inertia is the energy that is stored in the rotating masses of equipment electro-mechanically coupled to the system, e.g. generator rotors, fly wheels, turbine shafts.

## Derivation

Below is a basic derivation of power system rotational inertia from first principles, starting from the basics of circle geometry and ending at the definition of moment of inertia (and it's relationship to kinetic energy).

The length of a circle arc is given by:

- [math] L = \theta r [/math]

where [math]L[/math] is the length of the arc (m)

- [math]\theta[/math] is the angle of the arc (radians)
- [math]r[/math] is the radius of the circle (m)

A circular rotating mass therefore has a rotational velocity of:

- [math] v = \frac{\theta r}{t} [/math]

where [math]v[/math] is the rotational velocity (m/s)

- [math]t[/math] is the time it takes for the mass to rotate L metres (s)

Alternatively, rotational velocity can be expressed as:

- [math] v = \omega r [/math]

where [math]\omega = \frac{\theta}{t} = \frac{2 \pi \times n}{60}[/math] is the angular velocity (rad/s)

- [math]n[/math] is the speed in revolutions per minute (rpm)

The kinetic energy of a circular rotating mass can be derived from the classical Newtonian expression for the kinetic energy of rigid bodies:

- [math] KE = \frac{1}{2} mv^{2} = \frac{1}{2} m(\omega r)^{2}[/math]

where [math]KE[/math] is the rotational kinetic energy (Joules or kg.m^{2}/s^{2} or MW.s, all of which are equivalent)

- [math]m[/math] is the mass of the rotating body (kg)

Alternatively, rotational kinetic energy can be expressed as:

- [math] KE = \frac{1}{2} I\omega^{2} [/math]

where [math]I = mr^{2}[/math] is called the **moment of inertia** (kg.m^{2})