transformer

a static device (with no moving parts) for transforming the magnitude of an AC voltage. The operation of a transformer is based on the phenomenon of electromagnetic induction.

A transformer consists of a primary winding, one or more secondary windings, and a ferromagnetic core, or magnetic circuit, which is usually closed (see Figure 1). All the windings are located on the magnetic circuit and are inductively linked (seeMUTUAL INDUCTANCE). Sometimes part of the primary winding serves as the secondary, or vice versa; such transformers are called autotransformers. The terminals of the primary (the transformer input) are connected to a source of AC voltage, and those of the secondary (the output) are connected to the consumers. The alternating current in the primary produces an alternating magnetic flux in the magnetic circuit. In real transformers, part of the magnetic flux is closed outside the magnetic circuit, thereby forming a leakage flux; in high-quality transformers, however, the leakage fluxes are small compared to the mutual flux (the flux in the magnetic circuit).

The mutual flux Φ₀ produces the electromotive forces (emf’s) e₁ and e₂ in the primary and secondary windings, respectively: e₁ = – w₁dΦ₀/dt, and e₂ = – w₂dΦ₀/dt, where w₁ and w₂ are the number of turns on the corresponding windings. The ratio e₁/e₂ = w₁/w₂ = k is called the turn ratio. The voltages, currents, and emf’s (disregarding the emf’s induced by the leakage fluxes) are associated by the relationships

u₁ + e₁ = i₁r₁

and

u₂ + i₂r₂ = e₂

where r₁ and r₂, u₁ and u₂, i₁ and i₂ are the resistances, voltages, and currents of the windings. If the voltage u₁ applied to the primary is sinusoidal, then the magnetic flux Φ₀ and the emf’s e₁ and e₂ will also be sinusoidal. Therefore, in the analysis of the operation of transformers it is convenient to consider the effective values of the emf’s E₁ and E₂, of the voltages U₁ and U₂, and of the currents I₁ and I₂. For the no-load condition (secondary open), disregarding the resistance of the primary and assuming that I₂ = 0, we will have U₁ + E₁ = 0 and U₂ = E₂, that is (without regard to sign),

The mutual magnetic flux under no-load conditions is produced by the relatively small magnetizing current (the no-load current I₀) in the primary. If the transformer is loaded (the secondary is connected to a load, and current is flowing through it), the magnetomotive force of the secondary (the product I₂w₂) is compensated by a corresponding increase in the magnetomotive force of the primary (I₁w₁ – I₀w₁), and the value of the mutual magnetic flux remains virtually the same as for the no-load condition (that is, the condition U₁ + E₁ = 0 is preserved). Thus, by neglecting the no-load current we obtain I₁w₁ ≈ I₂w₂.

Transformers were first used in 1876 by P. N. lablochkov in electric lighting circuits. In 1890, M. O. Dolivo-Dobrovol’skii developed a three-phase transformer. The subsequent development of transformers produced improvements in design, increases in power and efficiency, and improvement of winding insulation. As of the mid-1970’s, many types of transformers had become commonplace in various fields of technology.

Power transformers are the main type of transformer, and among these the most representative group is the double-wound power transformers, which are used on power lines: Power transformers raise the voltage of the current generated at electric power plants from 10–15 kilovolts (kV) up to 220–750 kV, thus making possible the transmission of electric power over aerial transmission lines for several thousand kilometers. At locations where electric power is consumed, the high voltage is stepped down to low voltages (220 V, 380 V, and so on) by other power transformers. The repeated transformation of the electric power requires a large number of power transformers, and therefore the total power of the transformers in the system is several times that of the sources and power users. High-capacity power transformers have an efficiency of 98–99 percent. Their windings are generally made of copper, and their magnetic circuits of cold-rolled sheets of electrical steel 0.5–0.35 mm thick that have high magnetic permeability and low hysteresis and eddy-current losses. The magnetic circuit and windings of power transformers are usually mounted in a tank filled with mineral oil, which is used to insulate and cool the windings. Such transformers—called oil-filled transformers—are generally located in the open, which requires improved insulation of the leads and hermetic sealing of the tank. Transformers without oil cooling are called dry transformers. For better heat dissipation, power transformers are equipped with a tubular radiator around which the air or, in some cases, water circulates. In lightning-proof transformers the windings are designed so as to avoid the appearance of dangerous voltages across the insulation. Sometimes two or three transformers are connected in series. In many cases transformers with load tap changing are used. Among the dry transformers, low-power transformers with a large number of secondary windings (multiwinding transformers) make up a broad class. They are frequently used in radio engineering apparatus and automatic systems.

In addition to power transformers, there are many types designed to measure high voltages and currents (for example, instrument transformers, voltage transformers, and current transformers), to reduce the level of interference on wire communication lines (negative booster transformers), to convert a sine voltage to a pulse voltage (peaking transformers), to convert current and voltage pulses (peak transformers), to isolate an AC current component, and to decouple and match parts of an electric circuit.

Radio-frequency transformers are used to transform high-frequency voltages; they are made with magnetodielectric magnetic circuits or without a magnetic circuit. In radio transmitters the power of such transformers reaches several hundred kilowatts.