James L. Kirtley Jr. is an electrical engineer whose work concerns electric machines and electric power systems. MIT's departmental profile identifies him as a professor emeritus of electrical engineering, with energy and robotics among his research areas.[ref]
Figure 1.
James L. Kirtley Jr., portrait in MIT Energy Initiative's 2016 interview
. Identified James Kirtley photograph linked from the institutional interview; served directly by MIT.
The engineering problem is to match a motor's behaviour to its application. MIT reported in 2016 that Kirtley worked on customized electric motors for the MIT Cheetah robot, where brief peaks of torque serve running and jumping. The same interview describes his interest in electric motors interacting with microgrids, particularly their dynamic behaviour during supply disturbances.[ref] A short burst and sustained operation place different demands on the system; the largest instantaneous output alone does not describe its operating role.
His AC Power Flow in Linear Networks by James L. Kirtley Jr. connects the phasor representation of electric potential difference and electric current to physical energy transfer. In its peak-amplitude convention, complex electrical power is . With RMS phasors and , this becomes . The complex conjugate ensures that the relative phase enters the active power.[ref]
For an original load example in sinusoidal steady state, take and electrical impedance , using RMS phasors and the passive sign convention: electric current enters the positive-potential terminal. A series resistor and inductor realize this model at the specified angular frequency when and . Then
Thus active power is 48 watts, reactive power is 64 vars, apparent power is 80 volt-amperes, and power factor is . Write and . The corresponding electric potential difference and electric current are
Multiplying and applying a trigonometric identity gives instantaneous power
Its cycle average is 48 watts, while its range is watts. The negative portions represent temporary return of stored energy from this ideal load; the electrical resistance still dissipates a positive average. A synchronized product of the two waveforms reveals this behaviour, whereas multiplying their root mean square magnitudes gives only the apparent power.
Figure 2.
A phase-shifted load returns energy during part of each cycle while absorbing positive average power
. Original 20 volt RMS example with impedance ohms. The voltage and current have power factor 0.6; their instantaneous product ranges from -32 to 128 watts and averages 48 watts. Values are illustrative rather than measured motor data. Details.

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