Transformers

A transformer is two or more coils of wire sharing a magnetic core. Alternating current in one coil makes a voltage appear in the other, higher or lower depending on how many turns each coil has, with no wire joining them. Transformers carry power to your street, run doorbells and furnace controls, and sit inside chargers and audio gear. This final article explains how they work, how to read, choose and test them, and why some are among the most dangerous parts a hobbyist can pick up.

About the analogies. Everyday comparisons appear only in shaded "Analogy" boxes beside the real physics, and each box says where the comparison stops working.

1. A short recap

2. What a transformer is

A transformer transfers AC power from one circuit to another through a shared magnetic field. Its essential parts are the primary winding, fed by the AC source; the secondary winding, which delivers energy to the load; and the core, the path for the magnetic field.[3] A step-up transformer raises voltage and a step-down transformer lowers it.[4] The same part can often do either, depending on which winding you feed.[5]

Cores suit the frequency: iron or laminated steel below about 20 kHz,[3] air or powdered iron above it,[1] and ferrite in switch-mode power supplies.[6]

Analogy: a bicycle's gears. Gears trade speed for force without creating energy. A transformer trades voltage for current the same way: step the voltage down by ten and the available current rises tenfold, with power (nearly) unchanged.

Where it breaks down: gears work on steady motion, but a transformer works only while its current keeps changing. And gears are mechanically linked, while a transformer's two sides need share no wire, which makes electrical isolation possible.

3. How it works

From changing flux to secondary voltage

AC in the primary makes a magnetic field that keeps growing, collapsing and reversing. The iron core concentrates it and carries it through the secondary, inducing an AC voltage there.[4] This is mutual inductance: changing current in one coil induces an emf (electromotive force, a source voltage) in the other.[7] The field shared by both windings is the mutual flux.[8] (Flux, written Φ, measures the total magnetic field passing through a coil.)

With no load, the primary draws only a small exciting current to magnetize the core.[9] It stays small because the primary's changing field induces a counter-voltage opposing the supply, the back-EMF of article 5.[10] (Recap: back-EMF.) Connect a load and secondary current flows; by Lenz's law its field cancels some of the flux, the counter-voltage drops, and the primary draws more current. That is how the load's demand reaches the source.[8]

How a transformer works A square laminated iron core carries a dashed loop showing the changing magnetic flux. A primary winding of nine turns on the left leg is connected to an AC supply labeled Vp. A secondary winding of four turns on the right leg is connected to a load resistor labeled Vs. The flux created by the primary passes through both windings. Text below gives the turns-ratio equation: Vs divided by Vp equals Ns divided by Np. Vp AC supply Load Vs Laminated iron core Primary: Np turns Secondary: Ns turns Changing magnetic flux shared by both Vs / Vp = Ns / Np
Figure 1. How a transformer works. AC in the primary drives a changing flux around the core, which induces a voltage in every turn of both windings. With fewer secondary turns, this one steps the voltage down. Sources: OpenStax; NEETS.[4]​[8]

Why steady DC does not work

Faraday's law needs a changing flux. Steady DC on the primary produces no change, so nothing is induced in the secondary.[4] Worse, the counter-voltage that limits primary current disappears, leaving only the wire's resistance; NEETS warns that even below-rated frequency raises winding current enough to cause damage.[1] (Recap: why a coil passes DC freely.) DC switched on and off does produce secondary pulses,[4] which is what switch-mode supplies exploit.

The turns ratio

The same flux passes through every turn of both windings, inducing the same voltage per turn, so voltage scales with turns:[4]

Vs / Vp = Ns / Np

where V is voltage, N the number of turns, and the subscripts mean secondary and primary. A transformer cannot create energy, so, ignoring losses, VpIp = VsIs, and current scales the other way: Is / Ip = Np / Ns. In OpenStax's example, a charger with a 200-turn primary on 120 V needs a 25-turn secondary for 15 V, and a 16 A charging current draws only 2 A from the outlet.[4]

Impedance transformation, briefly

Impedance is the AC version of resistance. Because a transformer changes voltage one way and current the other, a load on the secondary looks different from the primary side: it is reflected by the square of the turns ratio,[11]​[12] Zp = (Np / Ns)2 × Zs. An 8 Ω loudspeaker behind a 10:1 transformer looks like 102 × 8 = 800 Ω (calculated). Matching source to load this way maximizes power transfer.[1] A tube amplifier's output transformer, typically about 30:1, makes 8 Ω look like several thousand ohms[11] (302 × 8 = 7,200 Ω, calculated).

Losses and efficiency

Real transformers turn some power into heat in three ways:[13]

Efficiency is output power divided by input power. NEETS puts small equipment transformers at 80 to 90 percent and large utility units above 98 percent.[13] OpenStax says efficiency "often exceeds 99%."[4] U.S. rules require oil-filled single-phase distribution transformers of 10 to 833 kVA (kilovolt-amperes; see section 4) to reach 98.70 to 99.55 percent at half load.[14]

Frequency and core size

Written for transformers, Faraday's law becomes ERMS = 4.44 × N × A × f × B × 10−8 where A is the core's cross-section in cm2, f the frequency, and B the peak flux density in gauss, which must stay below saturation.[15] For a given voltage, higher frequency lets turns and core area shrink. West Coast Magnetics says higher frequency "permits fewer turns and a smaller core for the same power," until rising core and copper losses limit the gain.[6] Even 50 versus 60 Hz matters: Bicron says a 60 Hz-only transformer is 20 percent smaller than a 50/60 Hz one.[15]

4. Ratings and markings

A transformer's limits come from its construction: insulation sets the safe voltage of each winding, wire diameter sets the current, and power handling depends on how well heat escapes, which is why big ones use oil or cooling fins. The power rating is usually given in volt-amperes (VA), rated voltage times rated current, though it may be stated in watts.[1]

A real example: Hammond's 166J12 is rated 12.6 VA, 115 V 60 Hz in, 12.6 V center-tapped at 1 A out. The 166J12B, for 117 V 50/60 Hz, is larger in every dimension.[16] Check that 12.6 V × 1 A = 12.6 VA, and that the 6.3 V on each side of the tap is half of 12.6 V.

Reading a transformer rating A card lists the ratings of a Hammond 166J12 transformer: primary 115 volts 60 hertz; secondary 12.6 volts center-tapped at 1.0 amp; 12.6 volt-amperes; Class B insulation rated 130 degrees Celsius; hi-pot test 2,000 volts RMS. Leader lines link each line to an explanation: connect only to the stated voltage and frequency; the secondary figures are RMS at full load with 6.3 volts on each side of the center tap; VA is rated volts times rated amps; the insulation class is a temperature limit; the hi-pot voltage is the insulation test voltage. Part 166J12 PRI 115 V 60 Hz SEC 12.6 V C.T. 1.0 A 12.6 VA Class B insulation (130 °C) Hi-pot 2,000 V RMS Connect only to this voltage and frequency; below-rated frequency can overheat it RMS volts and amps at full load; the center tap gives 6.3 V on each side Rated volts × rated amps (VA, not watts) Hottest temperature the insulation is rated for Voltage used to test the insulation Values from Hammond’s published data; real labels vary in layout.
Figure 2. Reading a transformer's ratings, using the Hammond 166J12. The card layout is illustrative; the values come from Hammond's table.[16] The frequency note is from NEETS.[1]

5. Kinds of transformer

Common transformer types
TypeWhat it isIsolated?Typical use
Step-down / step-up powerSeparate windings with different turns[4]YesPower supplies, chargers, the grid
Isolation (1:1)Equal voltages in and out, shielded, hi-pot tested at 2 kV[18]YesTest benches
AutotransformerOne tapped winding serving as both primary and secondary[1]NoAdjustable voltage, voltage conversion
Center-tappedA tap at the middle of a winding[9]YesFull-wave rectifiers, 120/240 V service[19]
E-I laminatedStacked E- and I-shaped steel sheets ("shell core")[20]YesGeneral mains equipment
ToroidalWindings around a ring of coiled steel strip[15]YesAudio and medical gear: smaller, lighter, low stray field[21]
High-frequency ferriteSmall Mn-Zn ferrite core, run at tens or hundreds of kHz[6]YesSwitch-mode supplies, chargers[22]
AudioLaminated core for 15 Hz to 20 kHz, impedance matched[1]YesMicrophone inputs, tube amplifier outputs[11]
RF and balunAir or powdered-iron core above 20 kHz[1]VariesRadio, antenna feeds[23]
Current transformerThe measured conductor passes through the core as the primary[24]YesMetering and protection
Distribution (pole or pad-mount)Oil-filled,[25] about 8,000 V to 120/240 V[26]YesThe transformer serving your house

Isolation and autotransformers. An isolation transformer has equal input and output voltages and exists only to separate them; Hammond's bench unit adds an electrostatic shield, a 3 A primary breaker and a 2 kV hi-pot test.[18] An autotransformer uses one tapped coil, so input and output share conductors and there is no isolation.[1] That is why OSHA forbids drawing welding current through one from an AC supply above 80 V.[27]

E-I versus toroidal. NEETS calls the E-I "shell core" the most popular and efficient design.[20] A toroid winds the copper around a ring. Noratel calls toroids smaller and lighter, with "very low magnetic strayfields";[21] Bicron says they need about 10 percent of a laminated core's magnetizing current.[15] The catch is a switch-on surge, or inrush current, of 30 to 90 times operating current, so they need slow-blow fuses.[21]

E-I laminated and toroidal transformer construction Left: an E-I core built from stacked E-shaped steel sheets with I-shaped sheets across the top. The copper winding sits on the center leg of the E and fills the two windows on either side of it. Right: a toroidal core, a ring of wound steel strip, with the copper winding spread evenly all the way around the ring and two leads coming out. I-shaped sheets Winding oncenter leg E-shaped sheets E-I laminated (shell) core Ring of woundsteel strip Toroidal core Leads
Figure 3. E-I laminated and toroidal construction. Steel and copper colors are fixed; proportions simplified. Sources: NEETS; Bicron.[20]​[15]

High-frequency ferrite transformers. Switch-mode supplies chop rectified mains at high frequency so the core can shrink, and almost all use manganese-zinc ferrite, which has the lowest losses there.[6] The common low-power design is the flyback transformer: coupled coils on a gapped core that store energy, then release it to the secondary. Coilcraft calls it the most popular choice for low-cost isolated supplies up to about 120 W, including battery chargers.[22] (Recap: switching power supplies.)

Audio, RF and baluns. Audio transformers couple and match stages over 15 Hz to 20 kHz; RF transformers work above 20 kHz.[1] A balun (balanced-unbalanced) connects a balanced line, two conductors carrying equal and opposite currents such as ribbon cable, to an unbalanced one with one side grounded, such as coaxial cable. A 4:1 balun matches a 300 Ω antenna lead to a 75 Ω receiver input.[23]

Current transformers. A current transformer (CT) uses the measured conductor as its primary and feeds a meter a small proportional current, typically 1 or 5 A. Its secondary must never be open while current flows, or it develops dangerously high voltage; short its terminals before disconnecting the meter.[24]

Distribution transformers. The green box on a lawn is a pad-mount transformer. A single-phase unit steps about 8,000 V down to 120/240 V for homes; three-phase units for businesses step about 13,800 V down to 120/208 or 277/480 V.[26] Pole-mounted units do the same job overhead.[12] A 240/120 marking means one 240 V winding with a center tap: 240 V across the ends and 120 V from either end to the tap, which becomes the neutral.[19]

6. Transformer circuits

A turns-ratio worked example

Suppose you need 12 V AC from 120 V mains at up to 2 A. Using the equations above,[4] the turns ratio is 120 ÷ 12 = 10:1, so a 600-turn primary needs a 60-turn secondary. The rating must be at least 12 V × 2 A = 24 VA. An ideal transformer would draw 24 ÷ 120 = 0.2 A from the outlet, a tenth of the secondary current. At 90 percent efficiency, the top of NEETS's range for small transformers,[13] it draws 24 ÷ 0.9 ≈ 26.7 W, about 0.22 A. (All calculated.)

A classic linear power supply

The classic way to make DC from mains is a linear supply: transformer, bridge rectifier, filter capacitor and regulator (Figure 4). Here is one for 9 V DC at 0.5 A using the Hammond 166J12 from section 4 (all numbers calculated).

  1. Fuse. The primary carries about 12.6 VA ÷ 115 V ≈ 0.11 A. Control-transformer codes allow a primary-only fuse up to 300 percent of that, about 0.33 A, and recommend a time-delay type so the switch-on surge does not blow it.[28]
  2. Transformer. 12.6 V RMS peaks at 12.6 × 1.41 ≈ 17.8 V.[29] (On a 120 V outlet this 115 V part gives about 4 percent more.)
  3. Bridge rectifier. Each half-cycle passes through two diodes of up to about 1 V each in a GBU4 bridge,[30] leaving about 15.8 V peak. Hammond advises diodes rated above 1.4 × 12.6 ≈ 17.6 V reverse and twice the output current;[29] 1N4001s (50 V, 1 A) qualify.[31] (Recap: the bridge rectifier.)
  4. Capacitor. With 2,200 µF, ripple is about 0.5 ÷ (2 × 60 × 0.0022) ≈ 1.9 V, so the voltage dips to about 13.9 V. (Recap: the ripple formula.)
  5. Regulator. An LM7809 needs at least 2 V more at its input than its output, its dropout voltage:[32] 11 V. The 13.9 V dips leave 2.9 V of margin, and about 1 V even if the mains sags 10 percent. Hammond says to allow for low line voltage.[29]
  6. Heat. The regulator burns off the rest: (14.9 V average in − 9 V) × 0.5 A ≈ 2.9 W. A bare TO-220 package rises 54 °C per watt,[32] about 160 °C here, so it needs a heat sink.
  7. Transformer current. The capacitor recharges in short, steep pulses, so the secondary's RMS current exceeds the DC. For a capacitor-input bridge, Hammond gives DC current = 0.62 × secondary AC current.[29] So 0.5 A DC needs about 0.81 A AC, or 10.2 VA. The 1 A, 12.6 VA part covers it; a naive 9 V × 0.5 A = 4.5 W estimate would not.
A linear 9 volt power supply, worked through Six blocks in a row joined by arrows: mains at 120 volts AC through a time-delay fuse; a Hammond 166J12 transformer giving 12.6 volts RMS; a bridge rectifier that drops about 2 volts; a 2,200 microfarad filter capacitor; an LM7809 regulator dissipating about 2.9 watts; and a 9 volt, 0.5 amp load. Beneath each block a sketched waveform: a large sine wave of 170 volts peak; a small sine wave of 17.8 volts peak; full-wave humps peaking near 15.8 volts; a smoothed line with a sawtooth ripple between 13.9 and 15.8 volts; and a flat 9 volt line, noting the regulator needs 11 volts in. The load uses 4.5 watts. All values are calculated. Mains 120 V AC time-delay fuse Transformer 166J12 12.6 V RMS Bridge rectifier drops about 2 V Capacitor 2,200 µF smooths Regulator LM7809 about 2.9 W heat Load 9 V DC 0.5 A 170 V peak (120 V RMS) 17.8 V peak (rated load) about 15.8 V peak 13.9 to 15.8 V 1.9 V ripple steady 9.0 V needs 11 V in 9 V × 0.5 A = 4.5 W Calculated values; waveforms are sketches, not to scale.
Figure 4. The linear supply worked through in the text: 120 V mains to a regulated 9 V at 0.5 A. Factors from Hammond's rectifier guide and the LM7800 data sheet.[29]​[32]

Isolation, and why it matters for safety

One side of household mains, the neutral, is connected to earth, so touching the other, "hot," wire while standing on the ground sends current through you back to the source.[33] An isolated secondary has no connection to earth, so touching one of its wires completes no circuit. Isolation plus low voltage is why the output of a doorbell or furnace transformer is far less hazardous than the mains feeding it; the AT140A is listed as meeting the National Electrical Code's Class 2 requirements.[17] The insulation between windings is what protects you, and makers hi-pot test it; Hammond uses 2,000 V RMS.[16]

A 1:1 isolation transformer on a mains bench is different. Rod Elliott of Elliott Sound Products explains that touching one output wire may not hurt you, but touching both is as lethal as ever, and a ground-fault breaker (GFCI) on the input cannot see it, so it will not trip.[33] It is a tool for specific service jobs, not a safety blanket. An autotransformer gives no isolation at all.[1]

Isolating transformer versus autotransformer Left: schematic of a two-winding transformer. The mains feeds the primary coil; a separate secondary coil feeds the isolated output. Two lines between the coils show the iron core, and no wire joins the two sides; the insulation between them is hi-pot tested. Right: an autotransformer, one winding with a tap. The input connects across the whole winding and the output is taken between the tap and the bottom end, so input and output share a conductor and there is no isolation. Mains in Isolated out No wire joins the two sides; insulation is hi-pot tested Two-winding (isolating) In Out Tap One tapped winding; input and output share a conductor Autotransformer (not isolating)
Figure 5. An isolating transformer has separate windings; an autotransformer does not. Sources: Hammond; NEETS.[18]​[1]

Phasing and dot notation

Whether the secondary voltage rises with the primary or opposite to it depends on winding direction and connections. Schematics mark this with dots: dotted ends have the same instantaneous polarity.[10] Polarity matters when connecting windings in series or parallel.[11] A distribution transformer marked 120/240 has two 120 V windings for series (240 V) or parallel (120 V) connection.[19] Phased wrongly in series, the voltages cancel; in parallel, each winding drives current into the other, limited only by the wire's resistance.

Dot notation and a center-tapped winding Left: a transformer symbol with dots at the top end of both windings; sketched sine waves under the primary and secondary rise and fall together. Middle: the same symbol with the secondary dot at the bottom end; the secondary sine wave is upside down relative to the primary. Right: a center-tapped winding with terminals X1, X2 and X3. X2, the center tap, is the neutral; there are 120 volts from X1 to X2 and from X2 to X3, and 240 volts from X1 to X3. Primary Secondary Dots on the same end voltages in phase Primary Secondary Dots on opposite ends secondary inverted X1 X2 (neutral) X3 120 V 120 V 240 V from X1 to X3 Center tap
Figure 6. Dot notation shows which winding ends rise together. A 240/120 winding is center-tapped, giving 120 V on each side of the neutral. Sources: NEETS; NETA World Journal.[10]​[19]

7. Testing transformers

Winding resistance, power off. Unplug and discharge the circuit first; filter capacitors can hold charge. (Recap: stored charge.) Each winding should show continuity and fairly low resistance; an open reading means a broken winding. The low-voltage winding, with thicker wire, reads lower than the high-voltage one, which helps identify unmarked leads.[1] Compare with the data sheet or an identical part.

Insulation, power off. There should be no continuity between separate windings, or from any winding to the core or frame, but an ordinary meter tests only at low voltage. An insulation resistance tester (megohmmeter) applies hundreds or thousands of volts DC, often for about a minute. Fluke suggests at least 1 MΩ for equipment rated up to 1,000 V. These testers are themselves a shock hazard: use them only on de-energized equipment, and discharge the windings before and after.[34]

Secondary voltage, power on. This is a live-mains job, so do it only with a proper setup: transformer mounted, primary connections enclosed and insulated, a fuse in the primary, and the meter clipped to the secondary before power goes on. Keep one hand in your pocket, the old electricians' trick Fluke recommends.[34] Expect more than the rating with no load: the AT140A gives 27.0 V open-circuit.[17] Never try this on a microwave-oven or other high-voltage transformer.

Signs of failure. Some hum is normal: it comes from magnetostriction, tiny changes in the core steel's shape as it magnetizes, and heavy charging pulses make it worse.[15] Loud buzzing or unusual odors are warning signs; Tampa Electric asks people to report either from a pad-mount transformer.[25] Excess current overheats windings until the insulation breaks down for good.[1] A burnt smell, discolored wrapping, swelling or a primary fuse that keeps blowing means retire the part.

8. Everyday uses

Transformers on the grid Six boxes in a row joined by arrows: a power plant generating at over 10 kilovolts; a step-up transformer at the plant; transmission lines at over 200 kilovolts and up to 700 kilovolts; a substation stepping down to 5 to 13 kilovolts; a pole or pad-mounted transformer stepping about 8 kilovolts down to 120 and 240 volts; and a home using 120 and 240 volts. A sketched line beneath shows the voltage stepping up for transmission and then down in stages. A note says high voltage means low current and far less I squared R loss on long lines. Power plant generated at over 10 kV Step-up transformer at the plant Transmission over 200 kV, up to 700 kV Substation step-down to 5 to 13 kV Pole or pad transformer: about 8 kV to 120/240 V Home 120 V and 240 V Voltage (sketch, not to scale) High voltage means low current, so far less I²R loss on long lines
Figure 7. Transformers raise voltage for long-distance transmission and lower it in stages for use. Voltages from OpenStax and OPPD.[4]​[26]

9. A note on solar and battery systems

Solar panels and batteries produce DC, and an inverter turns it into grid-compatible AC.[40] Whether a transformer is involved depends on the design. A review in an IEEE journal explains that isolated grid-tied inverters use a high-frequency transformer on the DC side or a low-frequency one on the AC side. Transformerless inverters are cheaper, smaller and more efficient, and popular for homes, but must meet strict standards on ground leakage current.[41] Microinverters, small inverters at each panel,[40] are among the listed uses of flyback transformers,[22] but only a model's documentation says what it contains. Large plants connect through step-up transformers; at NREL's Flatirons site, the solar plant and battery system feed a 13.2 kV bus through 480 V to 13.2 kV transformers.[42] Closer to home, utility transformers work in both directions,[5] and the standard for small grid-tied inverters is to disconnect when a grid disturbance is long or large. Battery systems run through outages only if designed to.[40] For any particular system, the installer's documentation is the authority.

10. Safety

Transformers connect directly to lethal voltages, and some make far higher ones. Unplug before touching, never defeat a fuse or enclosure, and leave high-voltage transformers to trained technicians.

The primary side is mains, and mains kills. OSHA reports that 50 to 150 mA through the body can stop breathing and may kill, and 1,000 to 4,300 mA can stop the heart.[43] NEETS adds that skin resistance cannot be relied on even at 115 V: deaths from 30 V have been recorded, and body resistance can fall to 300 Ω or less.[44] At 120 V and 300 Ω that is 400 mA (calculated). Treat every primary terminal, fuse holder and switch as live until unplugged, and enclose them so they cannot be touched.

Microwave-oven transformers (MOTs) are extremely dangerous. Hobbyists salvage them for projects such as "fractal" wood burning, which drives high voltage across wet wood to burn branching patterns. A 2020 case report describes MOTs producing 1,000 to 15,000 V with a potentially fatal 500 to 2,000 mA, against a "let-go" limit of about 16 mA. It also counted 34 fractal-burning injuries in local news since 2016, 24 of them fatal, a death rate of about 71 percent.[45] Western Australia's energy regulator prosecuted a man who built one from microwave parts and jumper leads after watching online videos; a man using it was killed when he touched live parts. The regulator notes that the American Association of Woodturners linked 31 U.S. deaths in five years to the practice and banned it at its events.[46] Inside the oven, the high-voltage capacitor can also hold a lethal charge after unplugging. Technical Safety BC warns that such voltages "can easily bypass" ordinary insulated tools and meters, and that these parts "should not be used outside their intended application."[38] Do not salvage, power or experiment with them. (Recap: microwave capacitors.)

A stepped-up secondary can be more dangerous than the input. A step-up transformer turns an ordinary outlet into about 2,000 V in a microwave oven[38] or 100 kV in OpenStax's portable x-ray example,[4] far more lethal than its input and able to defeat insulation and tools rated for mains.[38]

Never back-feed. A transformer works in both directions. A generator plugged into house wiring without a transfer switch can feed the neighborhood transformer backward, and the transformer then steps the voltage up on the utility line.[5] OSHA warns this can energize wiring "for great distances" and electrocute utility workers.[47] After Hurricane Hugo hit Puerto Rico in 1989, an experienced lineman was electrocuted by a line believed dead that was being fed by portable generators nearby.[48] Use only a transfer switch installed by a licensed electrician.[5] The same physics applies on the bench: feed any winding of a transformer and every other winding becomes live, so never power a low-voltage winding from another source and assume the primary leads are dead.[5]

Fuse it. North American codes require overcurrent protection on control transformers, in the primary or in both windings, sized from the rated current, with time-delay fuses recommended.[28] Toroids need slow-blow fuses or an inrush limiter.[21] Never replace a fuse with a larger one, and never bypass a built-in thermal cutoff like the C905's.[37]

Isolation transformers protect equipment and test gear, not you. Touching both sides of the secondary is as lethal as touching mains, and a GFCI ahead of the transformer will not trip.[33] Never power more than one appliance from one bench isolation transformer.[33]

Other rules. Short a current transformer's secondary before opening it.[24] Stay clear of pad-mount transformers, report any that are open or leaking oil, and call before digging nearby.[25] If someone is being shocked, free them without endangering yourself: switch off the power, or push them clear with something dry and nonconducting.[44]

The whole story in brief

Wrapping up the series

That completes the eight-part Electronics path. Article 1 started inside the atom, with valence electrons, current, voltage and resistance. Article 2 explained why some materials conduct and how doping makes semiconductors. Article 3 controlled current with resistors. Article 4 stored charge in an electric field, and article 5 stored energy in a magnetic one. Article 6 joined p-type to n-type to make the one-way diode, and article 7 built switches and amplifiers from two junctions or an insulated gate. This article used article 5's magnetism to move power between circuits. Together they cover the parts inside almost every power supply and circuit board. A good next step is to put them to work with a microcontroller in the Microcontrollers pages.

Sources

All links were checked in October 2026. External links open in a new tab.

  1. U.S. Navy, NEETS Module 2, chapter 5, "Transformer Ratings" and types of transformer (Integrated Publishing reprint): https://tpub.com/neets/book2/5i.htm
  2. U.S. Navy, NEETS Module 7: Introduction to Solid-State Devices and Power Supplies (PDF): https://legacy.maritime.org/doc/neets/mod07.pdf
  3. U.S. Navy, NEETS Module 2: Introduction to Alternating Current and Transformers, chapter 5, "Basic Operation of a Transformer" (Integrated Publishing reprint): https://tpub.com/neets/book2/5a.htm
  4. OpenStax, College Physics 2e, 23.7 "Transformers": https://openstax.org/books/college-physics-2e/pages/23-7-transformers
  5. Wisconsin Department of Agriculture, Trade and Consumer Protection, "Generators": https://datcp.wi.gov/Pages/Publications/Generators231.aspx
  6. West Coast Magnetics, "SMPS Transformer Design Guide": https://www.wcmagnetics.com/resource/switchmode-power-supply-transformer-design/
  7. OpenStax, University Physics Volume 2, 14.1 "Mutual Inductance": https://openstax.org/books/university-physics-volume-2/pages/14-1-mutual-inductance
  8. U.S. Navy, NEETS Module 2, chapter 5, "Effect of a Load" and mutual flux (Integrated Publishing reprint): https://tpub.com/neets/book2/5g.htm
  9. U.S. Navy, NEETS Module 2, chapter 5, schematic symbols, taps and the no-load condition (Integrated Publishing reprint): https://tpub.com/neets/book2/5d.htm
  10. U.S. Navy, NEETS Module 2, chapter 5, "Producing a Counter EMF" and phase-indicating dots (Integrated Publishing reprint): https://tpub.com/neets/book2/5e.htm
  11. Bill Whitlock, "Audio Transformers," chapter from Handbook for Sound Engineers, 3rd ed. (Jensen Transformers, PDF): https://www.jensen-transformers.com/wp-content/uploads/2014/09/Audio-Transformers-Chapter.pdf
  12. OpenStax, University Physics Volume 2, 15.6 "Transformers": https://openstax.org/books/university-physics-volume-2/pages/15-6-transformers
  13. U.S. Navy, NEETS Module 2, chapter 5, power relationship, transformer losses and efficiency (Integrated Publishing reprint): https://tpub.com/neets/book2/5h.htm
  14. U.S. Code of Federal Regulations, 10 CFR 431.196, energy conservation standards for distribution transformers (eCFR): https://www.ecfr.gov/current/title-10/chapter-II/subchapter-D/part-431/subpart-K/section-431.196
  15. Bicron Electronics, "Toroidal Power Transformers Technical Guide": https://www.bicronusa.com/resources/toroidal-power-transformers-technical-guide/
  16. Hammond Manufacturing, 166 Series low-voltage power transformers (0.63 to 288 VA), product page and table: https://www.hammfg.com/electronics/transformers/power/166
  17. Honeywell (Resideo), AT120A, AT140A, AT150A, AT175A Universal Transformers installation instructions, form 69-0251 (PDF): https://fwwebbimage.fwwebb.com/ProductInfo/69-0251-resideo.pdf
  18. Hammond Manufacturing, 171C Plug-In Isolation Transformers (115 VAC to 115 VAC) data sheet (PDF): https://www.hammfg.com/files/parts/pdf/171C.pdf
  19. Ben Gulick, "Guide to Low-Voltage Distribution Systems," NETA World Journal, May 2025: https://netaworldjournal.org/2025/05/bengulick/summer-2025-training-talk/guide-to-low-voltage-distribution-systems/
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