http://www.cwhdallas.com/tetrode-tubes/
Tetrode Tubes
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| 6P1P (~6AQ5 6V6), Svetlana Audiofiles Tetrode Tubes 8 pcs NOS | ![]() |
0 Bid | US $9.99 | 14h 4m |
| 6E5P Audiophile Tetrode Tubes Lot of 4 NOS | ![]() |
0 Bid | US $9.00 | 14h 7m |
| 6E6P-DRY/DRU Audiophile Tetrode Tubes. GOLD pins. 2pcs NOS | ![]() |
0 Bid | US $30.00 | 16h 57m |
| Strong Vintage RAYTHEON ER 224 Radio Vacuum Tube - Tetrode MIB NIP NOS | ![]() |
0 Bid | US $9.95 | 18h 26m |
| 1 Tung Sol 32 Tetrode Tube ~ For Radio ~ Tested! | ![]() |
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US $9.95 | 18h 54m |
| Eimac 4-125A Tetrode Vintage Vacuum Tube, Made in USA | ![]() |
0 Bid | US $9.99 | 21h 26m |
| RCA 5022 4-250A Power Tetrode Vacuum Tube, Made in USA | ![]() |
0 Bid | US $29.99 | 21h 26m |
| GU-74B = 4CX800A 4CX-800A SVETLANA TETRODE. LOT OF 2 NEW TUBES. FREE SHIPPING! | ![]() |
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US $299.00 | 28d 11h 28m |
| ART-13 Transmitting Vacuum Tube 813 Military Hi-Power Tetrode Excellent Cond. | ![]() |
1 Bid | US $9.99 | 1d 21h 37m |
| 6P3S-E/ 6L6 / 6L6GS / 5881 X 2pc.01/90`Output Beam Tetrode Tubes.NOS.NIB. | ![]() |
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US $15.00 | 20d 3h 46m |
| 6E15P HIGH VOLTAGE TETRODE TUBES. NOS. LOT of 8 | ![]() |
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US $7.95 | 22d 6h 44m |
| 6R3S 6R3S-1 Russian Double Power Tetrode Tube 10ps. | ![]() |
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US $74.99 | 25d 7h 54m |
| Two Type 24 Tung-Sol Receiving Tetrode Amplifier Vacuum Tubes | ![]() |
0 Bid | US $3.00 | 2d 18h 42m |
| (1) NOS NIB & (1) NOS Testing WH- 860 Tetrode Radio Transmitter Tubes | ![]() |
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US $75.00 | 2d 21h 36m |
| 6P3S tube. Output beam tetrode. Analouge 6L6 6L6GT NOS. 8 pcs | ![]() |
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US $27.99 | 22d 23h 57m |
| 6P6S tube. Output beam tetrode. 6V6 = 6AY5 = 587 NOS. 25 pcs | ![]() |
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US $64.99 | 13d 3h 9m |
| GU-74B = 4CX800A 4CX-800A SVETLANA TETRODE. 1 NEW TUBE | ![]() |
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US $137.00 | 10d 7h 54m |
| 6P42S (ca. 6P45S EL509 6KG6 ) output beam tetrode tube, Russian made, NOS QTY-2 | ![]() |
1 Bid | US $24.00 | 3d 13h 32m |
| GI 30 double pulse beam tetrode tube, Russian made, NOS QTY-2 | ![]() |
0 Bid | US $10.00 | 3d 13h 48m |
| Tube Socket For BEAM TETRODE G-807 G807 1625 5933,C51 | ![]() |
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US $3.99 | 17d 58m |
| 2 NOS/NIB RUSSIAN TUBES DOUBLE BEAM TETRODE GU-32/832 | ![]() |
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US $8.00 | 9d 21h 26m |
| G-807 / 807 / Beam Tetrode Tubes Lot of 4 | ![]() |
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US $17.95 | 14d 22h 50m |
| 6P6S = 6V6 = 6AY5 Russian Reflector Tetrode tube. NOS. Lot of 2. SAME DATE. | ![]() |
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US $6.00 | 6d 5h 14m |
| Western Electric 701A Radio Transmitting Tetrode Tube * NICE * | ![]() |
2 Bids | US $1.31 | 2d 19h 37m |
| 1 pieces of untested 6P44S / EL500 TETRODE tube | ![]() |
0 Bid | US $3.99 | 4d 2h 33m |
| 5 pieces of untested 6P13S = EL36 RUSSIAN TETRODE tube s | ![]() |
0 Bid | US $7.99 | 4d 2h 50m |
| GU 13 ( GU-13 ) Russian tube TETRODE Lot 1pc NOS tested | ![]() |
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US $45.99 | 27d 8h 53m |
| 6P6S tube. Output beam tetrode. 6V6 = 6AY5 = 587 NOS. 4 pcs | ![]() |
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US $14.99 | 23d 1h 20m |
| 6E5P Russian TETRODE TUBES LOT of 4 BOXED NEW | ![]() |
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US $8.56 | 22d 6h 41m |
| 6P1P-EV / 6AQ5 / EL90 output beam tetrode tubes SVETLANA. 2 pcs | ![]() |
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US $3.99 | 22d 6h 34m |
| 6E6P-DRY/DRU Audiophile Tetrode Tubes. GOLD pins. 2pcs NOS | ![]() |
0 Bid | US $30.00 | 4d 9h 21m |
| VINTAGE 6E5P Russian Audiophile Tetrode tubes NIB! NOS! QTY-16 | ![]() |
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US $29.99 | 28d 13h 2m |
| 6P3S tube. Output beam tetrode. Analouge 6L6 6L6GT NOS. 4 pcs | ![]() |
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US $14.99 | 22d 23h 57m |
| ^ Vintage Admiral (GE made) 6Y6G power tetrode vacuum tube,tested great!,6Y6,ST | ![]() |
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US $7.95 | 4d 10h 9m |
| 6P3S tube. Output beam tetrode. Analouge 6L6 6L6GT NOS. 2 pcs | ![]() |
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US $8.99 | 22d 23h 57m |
| GU-74B 74 B / 4CX800A Tetrode SVETLANA Tube 0.6kW. Lot of 2 pc. NOS! | ![]() |
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US $330.00 | 15d 22h 53m |
| GMI-83V (ГМИ-83В) RUSSIAN TUBE. POWER PULSE TETRODE-MODULATOR. NEW - LOT OF 1. | ![]() |
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US $47.00 | 26d 1h 54m |
| 6E15P HIGH VOLTAGE TETRODE TUBES NOS LOT OF 12 | ![]() |
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US $15.00 | 24d 23h 31m |
| NOS RCA 31LZ6 Electron Electronic Tube metal tetrode | ![]() |
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US $7.99 | 29d 23h 43m |
| 6CL8 Tube NOS DuMont USA Triode-Tetrode Frequency Conv | ![]() |
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US $2.95 | 29d 23h 12m |
| NOS GE 17JM6 Electron Electronic Tube metal tetrode NIB | ![]() |
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US $4.99 | 29d 22h 12m |
| NOS GE 21GY5 Electron Electronic Tube metal tetrode NIB | ![]() |
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US $2.99 | 29d 21h 48m |
| NOS GE 31LZ6 Electron Electronic Tube metal tetrode NIB | ![]() |
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US $9.99 | 29d 21h 32m |
| NOS GE 21JZ6 Electron Electronic Tube metal tetrode NIB | ![]() |
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US $5.99 | 29d 21h 21m |
| NOS GE 17JF6 Electron Electronic Tube metal tetrode NIB | ![]() |
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US $6.99 | 29d 21h 17m |
| NOS GE 36MC6 Electron Electronic Tube metal tetrode NIB | ![]() |
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US $14.99 | 29d 21h 12m |
| NOS GE 22KM6 Electron Electronic Tube metal tetrode NIB | ![]() |
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US $4.99 | 29d 20h 36m |
| NOS GE 26HU5 Electron Electronic Tube metal tetrode NIB | ![]() |
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US $9.99 | 29d 20h 33m |
| Tube, 2CY5, RCA Sharp-cut off Tetrode, Vhf amplifier (lot of 3) | ![]() |
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US $6.00 | 29d 20h 23m |
| Tube, 2CY5, RCA Sharp-cut off Tetrode, Vhf amplifier (lot of 2) | ![]() |
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US $5.00 | 29d 20h 21m |
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Hammond 1640SEA Single Ended "Classic", Ultra Linear Class-A Tube Output Transformer Sale Price: $160.00 |
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The Hammond 1640SEA is designed for single-ended tube output circuits. Includes a 40% screen grid tap for Ultra-Linear operation. Black matte finish. Audio watts: 30; Primary impedance: 1,250. |
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Manley Labs Neo-Classic 250 Watt Monoblock Amplifier List Price: $12,500.00 |
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Input sensitivity: 1V Gain: 32dB tetrode; 30dB in triode Input Impedance RCA: 116 Kohm @ 1KHz Input Impedance XLR: 270Kohm @ 1KHz; 20Kohms @ 20KHz; 38Kohm @ 20Hz Noise Floor: Tetrode: -67dB; Triode -65dB typical S/N Ratio: -80 dB Dynamic Range: 96dB Flat frequency response: 10 Hz - 30 KHz continuous Power Consumption: 30 Watts in "Ever-Warm" Full power (tetrode): 500W Full power (triode): 275W Factory set for 100V, 120V or 220-240VAC operation for original destination country's mains voltage. Operating Mains Voltage changeable with power transformer re-wiring and fuse value change. Mains Voltage Frequency: 50~ 60Hz Dims: W=19", D=13", H=9" Shipping weight: 82 lbs. each |
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High power Audio Beam Tetrode List Price: $140.00 |
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High Quality Audio Power Tube |
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Power Vacuum Tubes Handbook, Third Edition (Electronics Handbook Series) List Price: $149.95 Sale Price: $128.67 |
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Providing examples of applications, Power Vacuum Tubes Handbook, Third Edition examines the underlying technology of each type of power vacuum tube device in common use today. The author presents basic principles, reports on new development efforts, and discusses implementation and maintenance considerations. Supporting mathematical equations and extensive technical illustrations and schematic diagrams help readers understand the material.Translate Principles into Specific Applications This one-stop reference is a hands-on guide for engineering personnel involved in the design, specification, installation, and maintenance of high-power equipment utilizing vacuum tubes. It offers a comprehensive look at the important area of high-frequency/high-power applications of microwave power devices, making it possible for general principles to be translated into specific applications. Coverage includes power grid tubes—triodes, tetrodes, and pentodes—as well as microwave power tubes such as klystrons, traveling wave tubes, gyrotrons, and other high-frequency devices. These vacuum tubes are used in applications from radio broadcasting to television, radar, satellite communications, and more. Explore a Wide Variety of Methods in Power Vacuum Tube Design This third edition includes updates on vacuum tube technology, devices, applications, design methods, and modulation methods. It also expands its scope to cover properties of materials and RF system maintenance and troubleshooting. Explaining difficult concepts and processes clearly, this handbook guides readers in the design and selection of a power vacuum tube-based system. What’s New in This Edition Includes two new chapters on properties of materials and RF system maintenance and troubleshooting Contains updates and additions in most chapters Identifies key applications for commercial and scientific research Examines the frontiers of materials science directly impacting construction, reliability, and performance Reviews methods of power tube design for more efficient, longer-lasting tubes Features updated illustrations throughout to clarify and explain fundamental principles and implementation considerations |
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Power Vacuum Tubes Handbook, Second Edition (Electronics Handbook Series) List Price: $199.95 Sale Price: $162.40 |
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Providing examples of applications, this handbook examines the underlying technology of each type of power vacuum tube device in common use today. The author reports on new development efforts and explains the benefits of specific work. Basic principles are discussed, and supporting mathematics are included to clarify the material presented. Extensive technical illustrations and schematic diagrams aid the reader in understanding the maxims of the subject.What's New in the Second Edition?Reviews the latest in new vacuum tube technology - new devices and refinements of existing devices that extend power and frequency capabilitiesIdentifies new applications for commercial and scientific researchExamines new frontiers on materials science - directly impacting construction, reliability, and performanceOutlines new methods of power tube design - yielding more efficient, lasting tubesDescribes new modulation methods affecting power tube design and application, including digital technologies |
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Basic Electronics, Volume 2: Introduction to amplifiers; The Triode Tube; Tetrodes & Pentodes; Audio Voltage & Power Amplifiers |
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Radio transmitter design
Radio transmitter design is a complex topic which can be broken down into a series of smaller topics. A radio communication system requires two tuned circuits each at the transmitter and receiver, all four tuned to the same frequency. The transmitter is an electronic device which, usually with the aid of an antenna, propagates an electromagnetic signal such as radio, television, or other telecommunications.
Methods
At the beginning of the 20th century, there were four chief methods of arranging the transmitting circuits:
The transmitting system consists of two tuned circuits such that the one containing the spark-gap is a persistent oscillator; the other, containing the aerial structure, is a free radiator maintained in oscillation by being coupled to the first (Nikola Tesla and Guglielmo Marconi).
The oscillating system, including the aerial structure with its associated inductance-coils and condensers, is designed to be both a sufficiently persistent oscillator and a sufficiently active radiator (Oliver Joseph Lodge).
The transmitting system consists of two electrically coupled circuits, one of which, containing the air-gap, is a powerful but not persistent oscillator, being provided with a device for quenching the spark so soon as it has imparted sufficient energy to the other circuit containing the aerial structure, this second circuit then independently radiating the train of slightly damped waves at its own period (Oliver Joseph Lodge and Wilhelm Wien).
The transmitting system, by means either of an oscillating arc (Valdemar Poulsen) or a high-frequency alternator (Rudolf Goldschmidt), emits a persistent train of undamped waves interrupted only by being broken up into long and short groups by the operator's key.
Frequency synthesis
Fixed frequency systems
For a fixed frequency transmitter one commonly used method is to use a resonant quartz crystal in a Crystal oscillator to fix the frequency. Where the frequency has to be variable, several options can be used.
Variable frequency systems
An array of crystals used to enable a transmitter to be used on several different frequencies; rather than being a truly variable frequency system, it is a system which is fixed to several different frequencies (a subset of the above).
Variable-frequency oscillator (VFO)
Phase-locked loop frequency synthesiser
Direct digital synthesis
Frequency multiplication
Frequency doubler
A basic design for a frequency doubler (screen grids, bias supplies and other elements are not shown).
Frequency tripler
A basic design for a frequency tripler (screen grids, bias supplies and other elements are not shown).
For VHF transmitters, it is often not possible to operate the oscillator at the final output frequency. In such cases, for reasons including frequency stability, it is better to multiply the frequency of the free running oscillator up to the final, required frequency.
If the output of an amplifier stage is tuned to a multiple of the frequency with which the stage is driven, the stage will give a larger harmonic output than a linear amplifier. In a push-push stage, the output will only contain even harmonics. This is because the currents which would generate the fundamental and the odd harmonics in this circuit (if one valve was removed) are canceled by the second valve. In the diagrams, bias supplies and neutralization measure have been omitted for clarity. In a real system, it is likely that tetrodes would be used, as plate-to-grid capacitance in a tetrode is lower, thereby reducing stage instability.
In a push-pull stage, the output will contain only odd harmonics because of the canceling effect.
Frequency mixing and modulation
The task of many transmitters is to transmit some form of information using a radio signal (carrier wave) which has been modulated to carry the intelligence. A few rare types of transmitter do not carry information: the RF generator in a microwave oven, electrosurgery, and induction heating. RF transmitters that do not carry information are required by law to operate in an ISM band.
AM modes
In many cases the carrier wave is mixed with another electrical signal to impose information upon it. This occurs in Amplitude modulation (AM). Amplitude Modulation: In Amplitude modulation the instantaneous change in the amplitude of the carrier Frequency with respect to the amplitude of the modulating or Base band signal.
Low level and high level
Low level
Here a small audio stage is used to modulate a low power stage, the output of this stage is then amplified using a linear RF amplifier.
Advantages
The advantage of using a linear RF amplifier is that the smaller early stages can be modulated, which only requires a small audio amplifier to drive the modulator.
Disadvantages
The great disadvantage of this system is that the amplifier chain is less efficient, because it has to be linear to preserve the modulation. Hence class C amplifiers cannot be employed.
An approach which marries the advantages of low-level modulation with the efficiency of a Class C power amplifier chain is to arrange a feedback system to compensate for the substantial distortion of the AM envelope. A simple detector at the transmitter output (which can be little more than a loosely coupled diode) recovers the audio signal, and this is used as negative feedback to the audio modulator stage. The overall chain then acts as a linear amplifier as far as the actual modulation is concerned, though the RF amplifier itself still retains the Class C efficiency. This approach is widely used in practical medium power transmitters, such as AM radiotelephones.
High level
Advantages
One advantage of using class C amplifiers in a broadcast AM transmitter is that only the final stage needs to be modulated, and that all the earlier stages can be driven at a constant level. These class C stages will be able to generate the drive for the final stage for a smaller DC power input. However, in many designs in order to obtain better quality AM the penultimate RF stages will need to be subject to modulation as well as the final stage.
Disadvantages
A large audio amplifier will be needed for the modulation stage, at least equal to the power of the transmitter output itself. Traditionally the modulation is applied using an audio transformer, and this can be bulky. Direct coupling from the audio amplifier is also possible (known as a cascode arrangement), though this usually requires quite a high DC supply voltage (say 30 V or more), which is not suitable for mobile units.
Types of AM modulators
A wide range of different circuits have been used for AM. While it is perfectly possible to create good designs using solid-state electronics, valved (tube) circuits are shown here. In general, valves are able to easily yield RF powers far in excess of what can be achieved using solid state. Most high-power broadcast stations still use valves.
Plate AM modulators
Anode modulation using a transformer.
An example of a series modulated amplitude modulation stage.
In plate modulation systems the voltage delivered to the stage is changed. As the power output available is a function of the supply voltage, the output power is modulated. This can be done using a transformer to alter the anode (plate) voltage. The advantage of the transformer method is that the audio power can be supplied to the RF stage and converted into RF power. With anode modulation using a transforme, the tetrode is supplied with an anode supply (and screen grid supply) which is modulated via the transformer. The resistor R1 sets the grid bias, both the input and outputs are tuned LC circuits which are tapped into by inductive coupling. In series modulated amplitude modulation, the tetrode is supplied with an anode supply (and screen grid supply) which is modulated by the modulator valve. The resistor VR1 sets the grid bias for the modulator valve, both the RF input (tuned grid) and outputs are tuned LC circuits which are tapped into by inductive coupling.
When the valve at the top conducts more than the potential difference between the anode and cathode of the lower valve (RF valve) will increase. The two valves can be thought of as two resistors in a potentiometer.
Screen AM modulators
Screen AM modulator.
Under steady state conditions (no audio driven) the stage will be a simple RF amplifier where the grid bias is set by the cathode current. When the stage is modulated the screen potential changes and so alters the gain of the stage.
Other modes which are related to AM
Several derivatives of AM are in common use. These are
Single-sideband modulation
Main article: Single-sideband modulation
SSB, or SSB-AM single-sideband full carrier modulation, is very similar to single-sideband suppressed carrier modulation (SSB-SC)
Filter method
Using a balanced mixer a double side band signal is generated, this is then passed through a very narrow bandpass filter to leave only one side-band. By convention it is normal to use the upper sideband (USB) in communication systems, except for HAM radio when the carrier frequency is below 10 MHz here the lower side band (LSB) is normally used.
Phasing method
This method is an alternative method for the generation of single sideband signals. One of the weaknesses of this method is the need for a network which imposes a constant 90o phase shift on audio signals throughout the entire audio spectrum. By reducing the audio bandwidth the task of designing the phaseshift network can be made more easy.
Imagine that the audio is a single sine wave E = E sine (t)
The audio signal is passed through the phase shift network to give two identical signals which differ by 90o.
So as the audio input is a single sine wave the outputs will be
and
These audio outputs are mixed in non linear mixers with a carrier, the carrier drive for one of these mixers is shifted by 90. The output of these mixers is combined in a linear circuit to give the SSB signal.
Vestigial-sideband modulation
Main article: Vestigial-sideband modulation
Vestigial-sideband modulation (VSB, or VSB-AM) is a type of modulation system commonly used in analogue TV systems. It is normal AM which has been passed through a filter which reduces one of the sidebands. Typically, components of the lower sideband more than 0.75 MHz or 1.25 MHz below the carrier will be heavily attenuated.
Morse
Strictly speaking the commonly used 'AM' is double-sideband full carrier. Morse is often sent using on-off keying of an unmodulated carrier (Continuous wave), this can be thought of as an AM mode.
FM modes
Angle modulation is the proper term for modulation by changing the instantaneous frequency or phase of the carrier signal. True FM and phase modulation are the most commonly employed forms of analogue angle modulation.
Direct FM
Direct FM (true Frequency modulation) is where the frequency of an oscillator is altered to impose the modulation upon the carrier wave. This can be done by using a voltage-controlled capacitor (Varicap diode) in a crystal-controlled oscillator or frequency synthesiser. The frequency of the oscillator is then multiplied up using a frequency multiplier stage, or is translated upwards using a mixing stage, to the output frequency of the transmitter.
Indirect FM
Indirect FM solid state circuit.
Indirect FM employs a varicap diode to impose a phase shift (which is voltage-controlled) in a tuned circuit that is fed with a plain carrier. This is termed phase modulation. The modulated signal from a phase-modulated stage can be understood with an FM receiver, but for good audio quality, the audio is applied to the phase modulation stage. The amount of modulation is referred to as the deviation, being the amount that the frequency of the carrier instantaneously deviates from the centre carrier frequency.
In some indirect FM solid state circuits, an RF drive is applied to the base of a transistor. The tank circuit (LC), connected to the collector via a capacitor, contains a pair of varicap diodes. As the voltage applied to the varicaps is changed, the phase shift of the output will change.
Phase modulation is mathematically equivalent to direct Frequency modulation with a 6dB/octave high-pass filter applied to the modulating signal. This high-pass effect can be exploited or compensated for using suitable frequency-shaping circuitry in the audio stages ahead of the modulator. For example, many FM systems will employ pre-emphasis and de-emphasis for noise reduction, in which case the high-pass equivalency of phase modulation automatically provides for the pre-emphasis. Phase modulators are typically only capable of relatively small amounts of deviation while remaining linear, but any frequency multiplier stages also multiply the deviation in proportion.
Sigma-delta modulation ()
RF power amplifiers
Valves
For high power systems it is normal to use valves, please see Valve RF amplifier for details of how valved RF power stages work.
Advantages of valves
Good for high power systems
Electrically very robust, they can tolerate overloads for minutes which would destroy bipolar transistor systems in milliseconds
Disadvantages of valves
Heater supplies are required for the cathodes
High voltages (risk of death) are required for the anodes
Valves often have a shorter working life than solid state parts because the heaters tend to fail
Solid state
For low and medium power it is often the case that solid state power stages are used. For higher power systems these cost more per watt of output power than a valved system.
Linking the transmitter to the aerial
The majority of modern transmitting equipment is designed to operate with a resistive load fed via coaxial cable of a particular characteristic impedance, often 50 ohms. To connect the aerial to this coaxial cable transmission line a matching network and/or a balun may be required. Commonly an SWR meter and/or an antenna analyzer are used to check the extent of the match between the aerial system and the transmitter via the transmission line (feeder). An SWR meter indicates forward power, reflected power, and the ratio between them.
See Antenna tuner and balun for details of matching networks and baluns respectively.
EMC matters
Main article: Electromagnetic compatibility
While this section was written from the point of view of an amateur radio operator with relation to television interference it applies to the construction and use of all radio transmitters, and other electronic devices which generate high RF powers with no intention of radiating these. For instance a dielectric heater might contain a 2000 watt 27 MHz source within it, if the machine operates as intended then none of this RF power will leak out. However, if the device is subject to a fault then when it operates RF will leak out and it will be now a transmitter. Also computers are RF devices, if the case is poorly made then the computer will radiate at VHF. For example if you attempt to tune into a weak FM radio station (88 to 108 MHz, band II) at your desk you may lose reception when you switch on your PC. Equipment which is not intended to generate RF, but does so through for example sparking at switch contacts is not considered here.
RF leakage (defective RF shielding)
Main article: RF shielding
All equipment using RF electronics should be inside a screened metal box, all connections in or out of the metal box should be filtered to avoid the ingress or egress of radio signals. A common and effective method of doing so for wires carrying DC supplies, 50/60 Hz AC connections, audio and control signals is to use a feedthrough capacitor. This is a capacitor which is mounted in a hole in the shield, one terminal of the capacitor is its metal body which touches the shielding of the box while the other two terminal of the capacitor are the on either side of the shield. The feed through capacitor can be thought of as a metal rod which has a dielectric sheath which in turn has a metal coating.
In addition to the feed through capacitor, either a resistor or RF choke can be used to increase the filtering on the lead. In transmitters it is vital to prevent RF from entering the transmitter through any lead such as an electric power, microphone or control connection. If RF does enter a transmitter in this way then an instability known as motorboating can occur. Motorboating is an example of a self inflicted EMC problem.
If a transmitter is suspected of being responsible for a television interference problem, then it should be run into a dummy load; this is a resistor in a screened box or can which will allow the transmitter to generate radio signals without sending them to the antenna. If the transmitter does not cause interference during this test, then it is safe to assume that a signal has to be radiated from the antenna to cause a problem. If the transmitter does cause interference during this test then a path exists by which RF power is leaking out of the equipment, this can be due to bad shielding. This is a rare but insidious problem and it is vital that it be tested for. Such leakage is most likely to occur on homemade equipment or equipment that has been modified. RF leakage from microwave ovens may also sometimes be observed, especially when the oven's RF seal has been compromised.
Spurious emissions
Early in the development of radio technology it was recognised that the signals emitted by transmitters had to be 'pure'. For instance Spark-gap transmitters were quickly outlawed as they give an output which is so wide in terms of frequency. In modern equipment there are three main types of spurious emissions.
The term spurious emissions refers to any signal which comes out of a transmitter other than the wanted signal. The spurious emissions include harmonics, out of band mixer products which are not fully suppressed and leakage from the local oscillator and other systems within the transmitter.
Harmonics
These are multiples of the operation frequency of the transmitter, they can be generated in a stage of the transmitter even if it is driven with a perfect sine wave because no real life amplifier is perfectly linear.
Avoiding harmonic generation
Note that B+ is the anode supply, C- is the grid bias. While the circuit shown here uses tetrode valves (for example 2 x 4CX250B) many designs have used solid state semiconductor parts (such as MOSFETS). Note that NC is a neutralization capacitor.
Note that B+ is the anode supply, C- is the grid bias. While the circuit shown here uses a tetrode valve (for example the 4CX250B) many designs have used solid state semiconductor parts (such as MOSFETS).
It is best if these harmonics are designed out at an early stage. For instance a push-pull amplifier consisting of two tetrode valves attached to an anode tank resonant LC circuit which has a coil which is connected to the high voltage DC supply at the centre (Which is also RF ground) will only give a signal for the fundamental and the odd harmonics.
Removal of harmonics with filters
In addition to the good design of the amplifier stages, the transmitter's output should be filtered with a low pass filter to reduce the level of the harmonics.
Detection
The harmonics can be tested for using an RF spectrum analyser (expensive) or with an absorption wavemeter (cheap). If a harmonic is found which is at the same frequency as the frequency of the signal wanted at the receiver then this spurious emission can prevent the wanted signal from being received.
Local oscillators and unwanted mixing products
Imagine a transmitter, which has an intermediate frequency (IF) of 144 MHz, which is mixed with 94 MHz to create a signal at 50 MHz, which is then amplified and transmitted. If the local oscillator signal was to enter the power amplifier and not be adequately suppressed then it could be radiated. It would then have the potential to interfere with radio signals at 94 MHz in the FM audio (band II) broadcast band. Also the unwanted mixing product at 238 MHz could in a poorly designed system be radiated. Normally with good choice of the intermediate and local oscillator frequencies this type of trouble can be avoided, but one potentially bad situation is in the construction of a 144 to 70 MHz converted, here the local oscillator is at 74 MHz which is very close to the wanted output. Good well made units have been made which use this conversion but their design and construction has been challenging, for instance in the late 1980s Practical Wireless published a design (Meon-4) for such a transverter . This problem can be thought of as being related to the Image response problem which exists in receivers.
Simple but poor mixer
One method of reducing the potential for this transmitter defect is the use of balance and double balanced mixers. If the equation is assumed to be
E = E1 E2
and is driven by two simple sine waves, f1 and f2 then the output will be a mixture of four frequencies
f1
f1+f2
f1-f2
f2
If the simple mixer is replaced with a balanced mixer then the number of possible products is reduced. Imagine that two mixers which have the equation {I = E1 E2} are wired up so that the current outputs are wired to the two ends of a coil (the centre of this coil is wired to ground) then the total current flowing through the coil is the difference between the output of the two mixer stages. If the f1 drive for one of the mixers is phase shifted by 180 then the overall system will be a balanced mixer.
Note that while this hypothetical design uses tetrodes many designs have used solid state semiconductor parts (such as MOSFETS).
E = K . Ef2 . Ef1
So the output will now have only three frequencies
f1+f2
f1-f2
f2
Now as the frequency mixer has fewer outputs the task of making sure that the final output is clean will be simpler.
Instability and parasitic oscillations
If a stage in a transmitter is unstable and is able to oscillate then it can start to generate RF at either a frequency close to the operating frequency or at a very different frequency. One good sign that it is occurring is if an RF stage has a power output even without being driven by an exciting stage. Another sign is if the output power suddenly increases wildly when the input power is increased slightly, it is noteworthy that in a class C stage that this behaviour can be seen under normal conditions. The best defence against this transmitter defect is a good design, also it is important to pay good attention to the neutralization of the valves or transistors.
See also
Radio portal
The Wikibook Electronics has a page on the topic of
Transmitter design
References
Citations and notes
^ Cheney, M., Uth, R., & Glenn, J. (1999). Tesla, master of lightning. New York: Barnes & Noble Books. Page 71.
^ Thompson, S. P. (1918). Elementary lessons in electricity and magnetism. New York: Macmillan. Page 662
General information
Radio Society of Great Britain. (2005). Radio communication handbook. Potters Bar, Hertfordshire [England]: Radio Society of Great Britain. ISBN 0-900612-58-4
Sleeper, M. B. (1922). Design data for radio transmitters and receivers. Everyday engineering series, [no.] 6. New York: Norman W. Henley Pub.
Bucher, E. E. (1920). The wireless experimenter's manual, incorporating How to conduct a radio club, describes parliamentary procedure in the formation of a radio club, the design of wireless transmitting and receiving apparatus, long distance receiving sets, vacuum tube amplifiers, radio telegraph and telephone sets, the tuning and calibration of transmitters and receivers, general radio measurements and many other features. New York: Wireless press.
Bucher, E. E. (1921). Practical wireless telegraphy; a complete text book for students of radio communication. New York [etc.]: Wireless Press.
Categories: Radio technology | Radio electronics | CommunicationHidden categories: Articles with trivia sections from August 2008 | Wikipedia articles in need of updating | Wikipedia articles needing rewrite from May 2009 | Wikipedia articles needing context from October 2009
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