August 1955 Popular Electronics[Table of Contents]
People old and young enjoy waxing nostalgic about and learning some of the history of early electronics. Popular Electronics was published from October 1954 through April 1985. All copyrights are hereby acknowledged. See all articles from Popular Electronics.
Basic transformer circuits have not changed in the nearly sixty years since this article was published in Popular Electronics. The applications have definitely changed, though, since active circuits of the day required a relatively low voltage (step-down) for vacuum tube cathode heaters, and at least one relatively high voltage (step-up) for biasing the tube plate. Most transformers for today's consumer applications perform a single step-down operation for 3.3 V, 5 V, 12 V, etc. In many applications, transformers are done away with altogether in favor of solid state rectifiers and regulators.
The hum of a transformer is a song of leashed power held in check by the skill of design and construction engineers. In some transformers it signals lethal voltages lying in wait for the first incautious move; in others it tells of gentle voltages applied to delicate tube filaments. In any case, we can learn to handle this versatile component by becoming familiar with the basic rules that govern its operation.
A power transformer-the simplest kind consists of two separate coils of insulated wire wound around a common core of silicon steel or some similar material that concentrates magnetic lines of force. As a fluctuating voltage (Ep in Fig. A) is impressed across the primary (pri.) coil, the pulsating magnetic field that results from the flow of primary current (Ip) cuts through the secondary turns (sec.) inducing a new voltage (Es) in this winding. If a load that can consume electrical power is connected as shown, then a secondary current (Is) flows through the load. In modern power transformers, practically all of the lines of force produced by the primary current, cut through the secondary winding; this is a matter of proper design and materials. When it occurs, the windings are said to be "closely coupled," a condition that results in most efficient operation.
It should be pointed out that transformers operate only on alternating current, since the process of inducing a voltage in the secondary winding depends on a change in the magnetic lines of force. Don't let anyone talk you into trying to locate a d.c. transformer! Most of the electrical power in this country has a frequency of 60 cycles per second, although some 25-cycle power is still in use in various localities. The secondary voltage, Es, may be found by applying this simple formula:
Suppose we have a transformer whose primary has 500 turns closely coupled to a 2000-turn secondary. What secondary voltage may we anticipate if the input to the primary is 120 volts? Substituting in the formula above:
Thus, this is a step-up transformer which boosts the input voltage to four times its original value. The fraction 4/1 is called the S:P turns ratio. Evidently, from the example given above, the turns ratio is equal to the fraction "Secondary turns/Primary turns" and may be used in place of it in the equation, so that:
Es = Ep x turns ratio
Take another example: a filament transformer (a step-down type) designed to operate on 120-volts primary input has a turns ratio of 1:20 (another way of writing 1/20). What secondary voltage will it produce? Using the second formula:
By exercising care in the design of the windings and the choice of the core, both transformers described in the foregoing paragraphs may be combined to form a standard multiple winding type as shown in Fig. B by winding both secondaries on the same frame as the primary.
Contrary to the convictions of many beginners, transformers don't give you something for nothing. Although it is true that a transformer can step up voltage, in the process of so doing it balances the score by taking more current from the lines than it provides to the load. No transformer can ever supply more power to the load from the secondary winding than is put into its primary winding. Under ideal conditions of 100 % efficiency, the secondary power may equal the primary power, but it can never exceed it. Ignoring power factor (to be discussed in a future issue) :
Ep x Ip = primary power
Es x Is = secondary power
Ep x Ip = Es x Is
This last equation can be rewritten as:
Ip = Is x Es/Ep
and may be used to find the amount of primary current that will be necessary to provide a given secondary current to a load when a given transformer is used. For instance, consider our first example of a transformer having a turns ratio of 4/1. Assume that this device is to operate a radio set which acts as a 100-milliampere load. How much primary current must flow to supply this current at 480 volts in the secondary?
Ip = 100 x 480/120
Ip = 100 x 4 = 400 ma.
Therefore, as the transformer quadruples the input voltage by its step-up action to provide an output voltage of 480 volts, the current taken from the lines by its primary winding is four times greater than that provided for the load's use. This "balancing" action is completely automatic and is dictated by a natural law of physics called "the conservation of energy." If we could invent a transformer that would provide more secondary power than that consumed by its primary, perpetual motion would be the easy step!
Electrostatic speakers are beginning to find their way into modern, medium-priced high-fidelity equipment. It seems a good idea, then, to review the principles of this unique kind of loudspeaker to see how it fits into the hi-fi picture of today.
An electrostatic speaker is nothing more than an elegant capacitor having one flexible and one rigid plate. The principle of its operation is quite simple. Audio voltages applied to the plates of the capacitor set up a varying electric field between them. Since this field contains more or less energy depending upon the amplitude of the potential differences, the flexible plate is caused to move in step with these varying potentials. The air in contact with the moving electrode is then set in motion at an audio rate and sound results.
A typical circuit in which an electrostatic speaker is used in combination with a PM cone speaker to form a "woofertweeter" arrangement is given in the figure. Capacitors, C1 and C2, and inductance, L1, form a cross-over network which feeds the high frequency audio to the electrostatic speaker while keeping the low frequency components directed toward the low-frequency cone speaker transformer.
Early models of electrostatic speakers had two big disadvantages: they could not reproduce the low audio frequencies well and they often suffered voltage breakdowns because of the poor quality of the dielectric materials available at that time. The first problem is avoided by confining operation of the electrostatic speaker to the approximate audio range of 6500 to 15,000 cycles per second. A low frequency speaker is then required, of course, to supplement the capacitor speaker, that is, to provide reproduction over the range of 20 or 30 cycles to 7000 cycles or so. The second problem no longer exists because of the excellence of the new polyvinyls and polyethylenes which can withstand relatively high voltages without puncturing.
Posted August 31, 2011