Vacuum Diode History Working Principle and Types of Vacuum Diode

History of Vacuum Diode

In November 16, 1904 first vacuum diode was invented by Sir John Ambrose Fleming and it is also called the Fleming valve, the first thermionic valve. In those days there was no existence of p-n junction in electronics field. A conceptual figure of vacuum diode is shown below. vacuum diode

How does vacuum tube diode work?

Here the vacuum diode works mostly like modern diode. But its size is larger. It consists of a vacuum container with cathode and anode inside. This cathode and anode are connected across a voltage source.

The anode is applied with positive voltage with respect to cathode. Generally it works on principle of thermo ionic emission. This cathode is heated by a filament. Hence electrons get emitted from cathode and attracted towards anode. If the positive voltage applied at the anode is not sufficient enough the electrons emitted from cathode due to hot filament are not sufficiently attracted by anode.
As a result one cloud of electrons i.e. negative charge is accumulated in the space between cathode and anode. This is called space charge. Due to this space charge the further emitted electrons get repealed and come back to the cathode. Hence virtually electron emission stops. No current flows through the circuit. vacuum tube diode If the applied voltage between anode and cathode is increased gradually then more and more space charge electrons comes to the anode and create vacant space for further emitted electrons. So with increase of voltage across anode and cathode the emission rate of electrons will be increased. At the same time the space charge is gradually vanished that is neutralized on the anode. Once for certain applied voltage between anode and cathode the entire space charge is vanished. There is no more obstruction for emission of electrons from the cathode. Then a beam of electrons start flowing freely from cathode to anode through the space. As a result, current flows from the anode to cathode. vacuum tube diode forward biased On the other hand if anode is made negative with respect to cathode there is no electron emission from it as it is cold not hot. Now the emitted electrons from heated cathode do not come to the anode. Due to repulsion of negative anode strong space charge will be accumulated between anode and cathode. Again due to repulsion of this space charge all further emitted electrons come back to the cathode hence no virtual emission takes place hence no current flows in the circuit. So, vacuum diode allows current to flow in one direction only. vacuum tube diode reversed biased Under reverse bias this vacuum diode does not work. This vacuum tube was the basic component of electronics throughout the first half of the twentieth century. It was available and common in the circuit of radio, television, radar, sound reinforcement, sound recording system, telephone, analog and digital computers, and industrial process control.

V-I Characteristics of Vacuum Diode

The V-I characteristics of a vacuum diode is shown below. V-I characteristics of a vacuum tube The size of space charge depends upon the emission of electrons from cathode during formation of space charge. The emission of electrons further depends upon the temperature at which the cathode is heated. Hence if temperature is increased the amount of space charge is also increased. So the anode voltage required to neutralize the space charge will also be more. Thus same vacuum diode will have different V-I characteristic graphs at different cathode temperatures. In the above figure we have shown only three of them. One graph for ToC, one for temperature more than ToC and one for temperature less than ToC. When anode voltage is gradually increased from zero the current from anode to cathode is proportionally increased. Since the space charge limits the emission from cathode, the current is proportionally increased with decrease of space charge strength. This zone of the characteristics is called space charge limiting region as shown in the figure. After space charge is vanished the electron emission becomes constant and is solely dependent upon temperature of the cathode. Here the current in the vacuum diode becomes saturated. When no voltage is applied to anode there should not be any current in the circuit but actual case is not like that. Because of statistical fluctuation in the velocity, some electrons are energetic enough to reach the anode even there is no voltage at anode. The small current caused by this phenomenon is known as splash current.

Use of Vacuum Tube Diodes

Gradually p-n junction semiconductor has come in the market and vacuum tubes got replaced by them. The most basic structure of vacuum tube is vacuum diode. Still today somewhere vacuum tubes are being used widely. These fields for application of the vacuum tubes are in
  • Atomic Clocks
  • Audio Systems
  • Car Dashboards
  • Cellular Telephone Satellites
  • Computer Monitors
  • DVD Players and Recorders
  • Electromagnetic Testing
  • Electron Microscopes
  • Gas Discharge Systems
  • Gas Lasers
  • Guitar Amplifiers
  • Ham Radio
  • High-speed Circuit Switching
  • Industrial Heating
  • Ion Microscopes
  • Ion Propulsion Systems
  • Lasers
  • LCD Computer Displays
  • Lighting
  • Microwave Systems
  • Microwave Ovens
  • Military Systems
  • Mobile Phone, Bluetooth and Wi-Fi Microwave Components
  • Musical Instrument Amplifiers
  • Particle Accelerators
  • Photo multiplier Tubes
  • Plasma Panel Displays
  • Plasma Propulsion Systems
  • Professional Audio Equipment
  • Radar Systems
  • Radio Communications
  • Radio Stations
  • Recording Studios
  • Solar Collectors
  • Sonar Systems
  • Strobe Lights
  • Satellite Ground Stations
  • Semiconductor Vacuum Electronic Systems
  • TV Stations
  • Vacuum Electron Devices
  • Vacuum Panel Displays

Types of Vacuum Diodes

The vacuum diode tubes are classified as
  1. Frequency range wise (audio, radio, microwave)
  2. Power rating wise (small signal, audio power)
  3. Cathode/filament type wise (indirectly heated, directly heated)
  4. Application wise (receiving tubes, transmitting tubes, amplifying or switching)
  5. Specialized parameters wise (long life, very low micro phonic sensitivity and low noise audio amplification)
  6. Specialized functions wise (light or radiation detectors, video imaging tubes)


Closely Related Articles PN Junction Diode and its CharacteristicsDiode | Working and Types of DiodeDiode CharacteristicsHalf Wave Diode RectifierFull Wave Diode RectifierDiode Bridge RectifierWhat is Zener Diode?Application of Zener DiodeLED or Light Emitting DiodePIN Photodiode | Avalanche PhotodiodeTunnel Diode and its ApplicationsGUNN DiodeVaractor DiodeLaser DiodeSchottky DiodePower DiodesDiode ResistanceDiode Current EquationIdeal DiodeReverse Recovery Time of DiodeDiode TestingMore Related Articles Amplifier Gain | Decibel or dB GainIntegrated Circuits | Types of ICRegulated Power SupplyLaser | Types and Components of LaserWork FunctionMobility of Charge CarrierWhat are Photo Electrons? Electron volt or eVEnergy Quanta | Development of Quantum Physics Schottky EffectHeisenberg Uncertainty PrincipleSchrodinger Wave Equation and Wave FunctionCyclotron Basic Construction and Working PrincipleSinusoidal Wave SignalCommon Emitter AmplifierRC Coupled AmplifierDifferential AmplifierWave Particle Duality PrincipleSpace ChargeMOSFET | Working Principle of p-channel n-channel MOSFETMOSFET CircuitsMOS Capacitor | MOS Capacitance C V CurveApplications of MOSFETMOSFET as a SwitchMOSFET CharacteristicsPower MOSFETHalf Wave RectifiersFull Wave RectifiersBridge RectifiersClamping CircuitTheory of SemiconductorIntrinsic SemiconductorExtrinsic SemiconductorsEnergy Bands of SiliconDonor and Acceptor Impurities in Semiconductor Conductivity of SemiconductorCurrent Density in Metal and Semiconductor Intrinsic Silicon and Extrinsic SiliconP Type SemiconductorN Type SemiconductorP N Junction Theory Behind P N JunctionForward and Reverse Bias of P N JunctionZener BreakdownAvalanche BreakdownHall Effect Applications of Hall EffectGallium Arsenide SemiconductorSilicon SemiconductorTypes of TransistorsBipolar Junction Transistor or BJTBiasing of Bipolar Junction Transistor or BJTTransistor BiasingTransistor CharacteristicsCurrent Components in a TransistorTransistor Manufacturing TechniquesApplications of Bipolar Junction Transistor or BJT | History of BJTTransistor as a SwitchTransistor as an AmplifierJFET or Junction Field Effect Transistorn-channel JFET and p-channel JFETApplications of Field Effect TransistorDIAC Construction Operation and Applications of DIACTRIAC Construction Operation and Applications of TRIACPhototransistorNew Articles Trees and Cotrees of Electric NetworkDifferentiatorIntegratorPhase Synchronizing Device or Controlled Switching DeviceDigital to Analog Converter or DACDifference Amplifier