Engineering & Technology · Electrical Power, Conversion & Machines
Fields, induction and electromechanical conversion
A moving conductor in a magnetic field can develop voltage, and a current-carrying conductor can experience force. These are linked descriptions of conversion. A generator under electrical load needs a corresponding mechanical input; a motor delivering motion needs a corresponding electrical input.
Electrical Circuits supplies current/voltage, power, rms, phase and ideal storage relations. Engineering Thermodynamics supplies energy balances, losses and system boundaries. This chapter introduces magnetic flux and pole count before using them, derives the simple machine/converter relations and labels every invented parameter. All diagrams and numerical cases are original teaching models. They do not specify equipment construction, protective settings, installation, switching or qualification.
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Relate magnetic force, induced voltage and mechanical/electrical power without treating a field as a continuing free energy supply.
Keep the field quantities distinct
Magnetic flux density B describes a field locally, in teslas. Magnetic flux Φ through a specified surface accounts for its field component normal to that surface; for uniform B it is BA cosθ, where θ is the angle between the field and the surface normal. The flux unit is the weber, equal to tesla square metres.
For a straight conductor of length l carrying current I in a uniform field, force magnitude is BIl sinα, where α is the angle between the current direction and field. Direction matters as well as magnitude. A magnetic field that is parallel to that conductor gives zero force in this ideal relation, even if its magnitude is large.
Calculate a rate, not just a stored field value
Faraday’s law connects induced emf to changing flux linkage. If N turns link the same flux, the emf is −N dΦ/dt under a consistent orientation convention. The sign expresses opposition to the flux change in the induced-current effect. A constant flux can be large while giving zero induced emf in the stationary ideal coil.
A change can come from changing field, changing area or changing orientation. The original figure gives a defined flux history and the corresponding interval-by-interval emf. Its abrupt slope changes are mathematical corners; no physical waveform detail at those instants is claimed. Nor does induced voltage alone establish current: the connected circuit also matters.
Close the conversion account
In a perpendicular moving-conductor model, speed u gives emf magnitude Blu. Combining this with force BIl gives EI=Fu. The same interaction power appears on the electrical and mechanical sides. For rotation, mechanical power is torque times angular speed, P=Tω, with ω in radians per second.
In real machines, conductor resistance, magnetic-material losses, friction, windage and electronics can consume power. Changing magnetic or mechanical stored energy also enters during a transient. Permanent magnets can provide an interaction field, but they do not eliminate the need for an energy account or make every machine using them lossless.
A model should specify which quantity is held constant. Prescribed current and prescribed motion may require external sources to supply force or voltage. Those sources must stay inside the explanation, even when the diagram concentrates on one conductor or coil.
Check two original conversion calculations
First, an ideal 80-turn stationary coil links flux rising linearly from 2 mWb to 5 mWb over 0.10 s. The rate is (0.005−0.002)/0.10=0.030 Wb/s, so induced emf is −2.4 V in the declared orientation. During the following constant-flux interval it is zero, away from the corner.
Separately, choose B=0.5 T, active conductor length 0.2 m, perpendicular current 3 A and motion at 2 m/s in the force direction. Force magnitude is 0.3 N and opposing motional-emf magnitude is 0.2 V. Electrical conversion power EI=0.6 W equals mechanical power Fu=0.6 W.
These mathematical values do not specify a complete motor, field-source consumption, resistance, thermal limit or construction method. They establish the consistency of the coupling term. Add losses and changing stored energy before interpreting the input/output performance of actual equipment.
Try the reasoning
Does a stationary ideal coil necessarily generate voltage whenever flux is nonzero?
Show the answer and reasoning
No. Induced emf depends on the rate of flux linkage change, not its magnitude alone.
Why does a loaded generator require mechanical effort?
Show the answer and reasoning
Electrical energy delivery is coupled to mechanical work and losses; the induced-current effect opposes the imposed change.
Does the 0.6 W equality prove a whole real machine is 100% efficient?
Show the answer and reasoning
No. It checks an ideal interaction term; real input and output include losses and possibly changing stores.
What to carry forward
Use force, flux rate and power as connected accounts. State the geometry, orientation and boundary of the conversion model.
References
Teaching resources and research supporting this lesson’s explanations and examples.
Samuel J. Ling, Jeff Sanny and William Moebs; OpenStax/Rice University3 sources
- University Physics Volume 2 — 11.4 Magnetic Force on a Current-Carrying ConductorSamuel J. Ling, Jeff Sanny and William Moebs; OpenStax/Rice UniversityTeaching resource
- University Physics Volume 2 — 13.1 Faraday’s LawSamuel J. Ling, Jeff Sanny and William Moebs; OpenStax/Rice UniversityTeaching resource
- University Physics Volume 2 — 13.3 Motional EmfSamuel J. Ling, Jeff Sanny and William Moebs; OpenStax/Rice UniversityTeaching resource