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| triode |
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A highly evacuated electron tube containing an anode, a cathode, and a control grid.
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tri·ode (trī'ōd') ![]() |
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| triode |
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| Computer Desktop Encyclopedia: triode |
A type of vacuum tube that is used in audio and radio amplifiers and oscillator circuits. It is like a diode with the addition of a wire mesh control grid between the cathode and plate (anode) that controls current flow. A filament heats the cathode enabling it to release electrons. When a small voltage is applied to the grid, the current flow between the cathode and plate is changed accordingly. In some triodes, the filament is the cathode. See diode, tetrode and magnetron.
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| WordNet: triode |
The noun has one meaning:
Meaning #1:
a thermionic vacuum tube having three electrodes; fluctuations of the charge on the grid control the flow from cathode to anode which making amplification possible
| Wikipedia: Triode |
A triode is an electronic amplification device having three active electrodes. The term most commonly applies to a vacuum tube (or valve in British English) with three elements: the filament or cathode, the grid, and the plate or anode. The triode vacuum tube is the first electronic amplification device.
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The original three-element device was patented in 1908 by Lee De Forest who developed it from his original two-element 1906 Audion. The Audion did provide amplification. However it was not until around 1912 that other researchers, while attempting to improve the service life of the audion, stumbled on the principle of the true vacuum tube. The name triode appeared later, when it became necessary to distinguish it from other generic kinds of vacuum tubes with more or fewer elements (eg diodes, tetrodes, pentodes etc.). The Audion tubes deliberately contained some gas at low pressure. The name triode is only applied to vacuum tubes which have been evacuated of as much gas as possible.
There was a parallel invention of the triode in charge of Austrian Robert von Lieben.
The principle of its operation is that, as with a thermionic diode, the heated cathode(either directly or indirectly by means of a filament) causes a space charge of electrons that may be attracted to the positively charged plate (anode in UK parlance) and create a current. Applying a negative charge to the control grid will tend to repel some of the (also negatively charged) electrons back towards the cathode: the larger the charge on the grid, the smaller the current to the plate. If an AC signal is superimposed on the DC bias of the grid, an amplified version of the AC signal appears in the plate circuit.
Although triodes are now largely obsolete in consumer electronics, having been replaced by the transistor, triodes continue to be used in certain high-end and professional audio applications, as well as in microphone preamplifiers and electric guitar amplifiers.
Some guitarists routinely drive their amplifiers to the point of saturation, in order to produce a desired distortion tone. Many people prefer the sound of triodes in such an application, since the distortion of a tube amplifier, which has a "soft" saturation characteristic, can be more pleasing to the ear than that of a typical solid-state amplifier, which through negative feedback is linear up to the limits of its supply voltage and then clips abruptly.
In triode datasheets, characteristics linking the anode current(Ia) to anode voltage (Va) and grid voltage (Vg) were usually given. From here, designer would choose the operating point of the particular triode.
In the example characteristic shown on the image, we can select our anode voltage Va=200 V. Next we can select grid DC voltage bias, let's use -1 V. This corresponds to the yellow curve on our graph. We can see that anode current of about 2.25 mA corresponds to this operating point.
In the class A triode amplifier, anode resistor would be connected between anode and the positive voltage source. If we select value of Ra=10000 Ohms, voltage drop on it will be
VRa=Ia×Ra=22.5 V,
if anode current of Ia=2.25 mA is chosen.
Now, if input voltage amplitude (at grid) changes from -1.5 V to -0.5 V (difference of 1 V), anode current will change from 1.2 to 3.3 mA (see image). This will result in anode resistor voltage drop changes from 12 to 33 V (difference of 21 V).
Since grid voltage changes from -1.5 V to -0.5 V, and anode resistor voltage drop from 12 to 33 V, amplification of signal resulted. Amplification factor is 21 - output voltage amplitude divided by input voltage amplitude.
This entry is from Wikipedia, the leading user-contributed encyclopedia. It may not have been reviewed by professional editors (see full disclaimer)
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