Module 12 - Modulation Principles
Navy Electricity and Electronics Training Series (NEETS)
Chapter 1:  Pages 1-21 through 1-30

Figure 1-14A. - Waveforms across two nonlinear impedances.

Figure 1-14B. - Waveforms across two nonlinear impedances.

If the two sine wave generators are of different frequencies, then the sum of the instantaneous values will appear as a complex wave across the impedances, as shown in figure 1-15, views (A) and (B). To determine the wave shape across each individual impedance, assume only one generator is connected at a

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time and compute the sine-wave voltage developed across each impedance for that generator input. Then, combine the instantaneous voltages (caused by each generator input) to obtain the complex waveform across each impedance. The nature of the impedance (resistive or reactive) will determine the shape of the complex waveform. Because the complex waveform is the sum of two individual sine waves, the composite waveform contains only the two original frequencies.

Figure 1-15A. - Sine-wave generators with different frequencies and linear impedances.

Figure 1-15B. - Sine-wave generators with different frequencies and linear impedances.

Linear impedances may alter complex waveforms, but they do not produce new frequencies. The output of one generator does not influence the output of the other generator.

TWO SINE WAVE GENERATORS and a Combination of LINEAR and NONLINEAR ImpedanceS

Figure 1-16 illustrates a circuit that contains two sine-wave generators (G1 and G2), linear impedance Z1, and nonlinear impedance Z2, in series. When a single sine-wave voltage is applied to a

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combined linear and nonlinear impedance circuit, the voltages developed across the impedances are complex waveforms.

Figure 1-16. - Sine-wave generators with a combination of impedances.

When two sine wave voltages are applied to a circuit, as in figure 1-16, nonlinear impedance Z2 reshapes the two sine-wave inputs and their harmonics, resulting in a very complex waveform.

Assume that nonlinear impedance Z2 will allow current to flow only when the sum of the two sine-wave generators (G1 and G2) has the polarity indicated. The waveforms present across the linear impedance will appear as a varying waveform. This will be a complex waveform consisting of:

   • a dc level

   • the two fundamental sine wave frequencies

   • the harmonics of the two fundamental frequencies

   • the sum of the fundamental frequencies

   • the difference between frequencies

The sum and difference frequencies occur because the phase angles of the two fundamentals are constantly changing. If generator G1 produces a 10-hertz voltage and generator G2 produces an 11-hertz voltage, the waveforms produced because of the nonlinear impedance will be as shown in the following list:

   • a 10-hertz voltage

   • an 11-hertz voltage

   • harmonics of 10 hertz and 11 hertz (the higher the harmonic, the lower its strength)

   • the sum of 10 hertz and 11 hertz (21 hertz)

   • the difference between 10 hertz and 11 hertz (1 hertz)

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Figure 1-17 illustrates the relationship between the two frequencies (10 and 11 hertz). Since the waveforms are not of the same frequency, the 10 hertz of view (B) and the 11 hertz of view (A) will be in phase at some points and out of phase at other points. You can see this by closely observing the two waveforms at different instants of time. The result of the differences in phase of the two sine waves is shown in view (C). View (D) shows the waveform that results from the nonlinearity in the circuit.

Figure 1-17A. - Frequency relationships.

Figure 1-17B. - Frequency relationships.

Figure 1-17C. - Frequency relationships.

Figure 1-17D. - Frequency relationships.

The most important point to remember is that when varying voltages are applied to a circuit which contains a nonlinear impedance, the resultant waveform contains frequencies which are not present at the input source.

The process of combining two or more frequencies in a nonlinear impedance results in the production of new frequencies. This process is referred to as heterodyning.

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SPECTRUM ANALYSIs

The heterodyning process can be analyzed by using SPECTRUM ANALYSIs (the display of electromagnetic energy arranged according to wavelength or frequency). As shown in figure 1-18, spectrum analysis is an effective way of viewing the energy in electronic circuits. It clearly shows the relationships between the two fundamental frequencies (10 and 11 hertz) and their sum (21 hertz) and difference (1 hertz) frequencies. It also allows you to view the Bandwidth (the amount of the frequency spectrum that signals occupy) of the signal you are studying.

Figure 1-18. - Spectrum analysis of heterodyned signal.

Typical HETERODYNING Circuit

Two conditions must be met in a circuit for heterodyning to occur. First, at least two different frequencies must be applied to the circuit. Second, these signals must be applied to a nonlinear impedance. These two conditions will result in new frequencies (sum and difference) being produced. Any one of the frequencies can be selected by placing a frequency-selective device (such as a tuned tank circuit) in series with the nonlinear impedance in the circuit.

Figure 1-19 illustrates a basic heterodyning circuit. The diode D1 serves as the nonlinear impedance in the circuit. Generators G1 and G2 are signal sources of different frequencies. The primary of T1, with its associated capacitance, serves as the frequency-selective device.

Figure 1-19. - Typical heterodyning circuit.

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The principles of this circuit are similar to those of the block diagram circuit of figure 1-16. Notice in figure 1-19 that the two generators are connected in series. Therefore, the resultant waveform of their combined frequencies will determine when the cathode of D1 will be negative with respect to the anode, thereby controlling the conduction of the diode. The new frequencies that are generated by applying these signals to nonlinear impedance D1 are the sum and difference of the two original frequencies. The frequency-selective device T1 may be tuned to whichever frequency is desired for use in later circuit stages. Heterodyning action takes place, intentionally or not, whenever these conditions exist. Heterodyning (MIXING) circuits are found in most electronic transmitters and receivers. These

transmitter and receiver circuits will be explained in detail later in this module.

Q-14. Define the heterodyne principle.

Q-15. What is a nonlinear impedance?

Q-16. What is spectrum analysis?

Q-17. What two conditions are necessary for heterodyning to take place?

Amplitude-MODULATED Systems

Amplitude modulation refers to any method of varying the amplitude of an electromagnetic carrier frequency in accordance with the intelligence to be transmitted by the carrier. The CARRIER frequency is a radio-frequency wave suitable for modulation by the intelligence to be transmitted. One form of this method of modulation is simply to interrupt the carrier in accordance with a prearranged code.

CONTINUOUS WAVE (CW)

The "on-off" KEYING of a continuous wave (CW) carrier frequency was the principal method of modulating a carrier in the early days of electrical communications. The intervals of time when a carrier either was present or absent conveyed the desired intelligence. This is still used in modern communications. When applied to a continuously oscillating radio-frequency source, on-off keying is referred to as CW signaling. This type of communication is sometimes referred to as an interrupted continuous wave (ICW).

Development

The use of a CW transmitter can be very simple. All that is required for the transmitter to work properly is a device to generate the oscillations, a method of keying the oscillations on and off, and an antenna to radiate the energy. Continuous wave was the first type of modulation used. It is still extensively used for long-range communications. When Marconi and others were attempting the transfer of intelligence between two points, without reliance on a conducting path, they employed the use of a practical coding system known as Morse code. You probably know that Morse code is a system of on-off keying developed for telegraph that is capable of passing intelligence over wire at an acceptable rate. Morse code consists only of periods of signal and no-signal.

Figure 1-20 is the International Morse code used with telegraphy and cw modulation. Each character in the code is made up of a series of elements referred to as DOTS or DASHES. These are short (dot) and long (dash) bursts of signal separated by intervals of no signal. The dot is the basic time element of the code. The dash has three times the duration of a dot interval. The waveforms for both are shown in figure 1-21. The elements within each character are separated by intervals of no signal with a time duration of one dot. The characters are separated by a no-signal interval equal in duration to one dash. Each interval

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during which signal is present is called the MARKING interval, and the period of no signal is called the SPACING interval. Figure 1-22 shows the relationships between the RF carrier view (A), the on-off keying waveform view (B), and the resultant carrier wave view (C).

Figure 1-20. - International Morse code.

Figure 1-21. - Dot and dash in radiotelegraph code.

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Figure 1-22A. - Essential elements of ON-ofF keying.

Figure 1-22B. - Essential elements of ON-ofF keying.

Figure 1-22C. - Essential elements of ON-ofF keying.

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Keying Methods

Keying a transmitter causes an RF signal to be radiated only when the key contacts are closed. When the key contacts are open, the transmitter does not radiate energy. Keying is accomplished in either the oscillator or amplifier stage of a transmitter. a number of different keying systems are used in Navy transmitters.

In most Navy transmitters, the hand telegraph key is at a low-voltage potential with respect to ground. a keying bar is usually grounded to protect the operator. Generally, a keying relay, with its contacts in the center-tap lead of the filament transformer, is used to key the equipment. Because one or more stages use the same filament transformer, these stages are also keyed. a class C final amplifier, when operated with fixed bias, is usually not keyed. This is because no output occurs when no excitation is applied in class C operation. Keying the final amplifier along with the other stages is not necessary in this case.

Oscillator KEYING. - Two methods of Oscillator KEYING are shown in figure 1-23. In view (A) the grid circuit is closed at all times. The key (K) opens and closes the negative side of the plate circuit. This system is called PLATE KEYING. When the key is open, no plate current can flow and the circuit does not oscillate. In view (B), the cathode circuit is open when the key is open and neither

grid current nor plate current can flow. Both circuits are closed when the key is closed. This system is called CATHODE KEYING. Although the circuits of figure 1-23 may be used to key amplifiers, other

keying methods are generally employed because of the high values of plate current and voltage

encountered.

Figure 1-23A. - Oscillator keying.

Figure 1-23B. - Oscillator keying.

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BlockED-GRID KEYING. - Two methods of BlockED-GRID KEYING are shown in figure

1-24. The key in view (A) shorts cathode resistor R1 allowing normal plate current to flow. With the key open, reduced plate current flows up through resistor R1 making the end connected to grid resistor Rg negative. If R1 has a high enough value, the bias developed is sufficient to cause cutoff of plate current. Depressing the key short-circuits R1. This increases the bias above cutoff and allows the normal flow of plate current. Grid resistor Rg is the usual grid-leak resistor for normal biasing.

Figure 1-24A. - Blocked-grid keying.

Figure 1-24B. - Blocked-grid keying.

The blocked-grid keying method in view (B) affords a complete cutoff of plate current. It is one of

the best methods for keying amplifier stages in transmitters. In the voltage divider with the key open, two- thirds of 1,000 volts, or 667 volts, is developed across the 200-kilohm resistor; one-third of 1,000 volts, or 333 volts, is developed across the 100-kilohm resistor. The grid bias is the sum of 100 volts and 333 volts, or 433 volts. This sum is below cutoff and no plate current flows. The plate voltage is 667 volts. With the key closed, the 200-kilohm resistor drops 1,000 volts. The plate voltage becomes 1,000 volts at the same time the grid bias becomes 100 volts. Grid bias is reduced enough so that the triode amplifier will conduct only on the peaks of the drive signal.

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