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Alternating Current Becomes Useful

The alternator and transformer turn a naturally reversing current into a practical power system

Alternating current was not a late discovery. Hippolyte Pixii's generator in 1832 naturally produced an alternating output as opposite magnetic poles passed the coil. A commutator was then used when a unidirectional output was wanted.

By the 1870s and 1880s, practical alternators were being built specifically to produce alternating current. The important new question was no longer whether AC could be generated. It was what useful devices could be built around it.

An alternator produces a voltage that repeatedly reverses polarity.

A transformer can then change the voltage without a rotating mechanical commutator.

The alternator

The basic alternator still follows Faraday's law. Relative motion between a magnetic field and coils changes the magnetic flux through the conductors and induces an EMF.

If the magnetic polarity seen by a coil repeatedly reverses as the machine rotates, the induced voltage also reverses. That is alternating current at the generator terminals.

rotation → changing magnetic flux → alternating EMF → AC output

The transformer was already hiding in Faraday's ring

Faraday's 1831 induction experiments had already shown that a changing current in one coil could induce a voltage in another coil. The later transformer turns that laboratory observation into a practical device.

In the early 1880s Lucien Gaulard and John Dixon Gibbs demonstrated transformer systems. In 1885, Károly Zipernowsky, Ottó Bláthy, and Miksa Déri developed the ZBD transformer system using closed magnetic cores and parallel distribution. In 1886, William Stanley demonstrated a practical transformer-based AC distribution system at Great Barrington, Massachusetts.

A transformer has no rotating shaft.
  • AC in the primary winding creates a changing magnetic flux.
  • The core guides much of that changing flux through the secondary winding.
  • The changing flux induces a voltage in the secondary.
  • The turns ratio determines whether the voltage is stepped up or stepped down.

Why changing voltage matters

For a given amount of power, raising the voltage allows the current to be reduced. Lower current means much less heating loss in a transmission wire because:

Pwire loss = I2R

A transformer therefore makes an important system possible: generate at one voltage, step it up for transmission, then step it down again near the load.

Measurement trail 17 — transformer turns ratio

For an ideal transformer, the voltage ratio approximately follows the turns ratio:

Vs / Vp = Ns / Np

A simple 10-to-1 step-down transformer

If the primary has 1000 turns and the secondary has 100 turns:

Ns / Np = 100 / 1000 = 0.1

With 1200 V applied to the primary, the ideal secondary voltage would be about:

Vs = 1200 V × 0.1 = 120 V

Real transformers have copper loss, core loss, leakage flux, heating, insulation limits, and regulation error, but the turns-ratio calculation is an excellent first ball-park estimate.

DC versus AC — important history, but the devices matter more here

The 1880s brought a famous commercial and technical struggle between competing power systems. That story matters, but LearnTronics does not need to turn it into the main event.

Our device trail is simpler:

generator → alternator → transformer → higher-voltage transmission → step-down transformer → useful load

AC still lacked one especially elegant device that DC systems already had: a simple, rugged motor without a commutator. The rotating magnetic field will soon solve that problem.