The junction field-effect transistor action. It was previously emphasized that one of the main properties of the bipolar transistor is that it is a current-controlled amplifying device; the output current is controlled by a small input current. In the case of the field-effect transistor (FET) it is the input voltage which controls the output current. The current drawn by the input is usually negligible. This is a great advantage where the signal comes from a device such as capacitor microphone or piezoelectric transducer, which is unable to supply a significant current. FET’s are basically of two types: the junction field-effect transistor (JFET) and the insulated gate field-effect transistor (IGFET). The latter is more commonly known by a name metal-oxide semiconductor field-effect transistor (MOSFET).
At a point along the bar a region of p-type silicon forms a p-n junction. In normal operation, the junction is reverse-biased. The lower contact on the bar is called the source and the upper contact the drain. The electron current flows from source to drain and is controlled by the voltage applied to the p-region called the gate.
An alternative type of construction is the p-channel device where the gate is made of n-type material.
The operation of the JFET depends upon variations in the size of the depletion layer at the reverse-biased gate junction. The p-type gate is much more heavily doped than the n-type bar, so that the depletion region exists almost entirely in the bar. The gate carries a negative bias voltage relative to the source which give rise to the particular shape of the depletion region: this is wider at the top than the bottom. The wider the depletion layer, the narrower the channel there is available for the flow of electrons from source to drain, since the depletion region itself being devoid of current carries, behaves like an insulator.
Unlike the bipolar transistor, the FET employs only majority carriers for its operation. It is therefore sometimes called the unipolar transistor and is less susceptible than the bipolar type to temperature changes and nuclear radiation.
The junction field-effect transistor action. It was previously emphasized that one of the main properties of the bipolar transistor is that it is a current-controlled amplifying device; the output current is controlled by a small input current. In the case of the field-effect transistor (FET) it is the input voltage which controls the output current. The current drawn by the input is usually negligible. This is a great advantage where the signal comes from a device such as capacitor microphone or piezoelectric transducer, which is unable to supply a significant current. FET’s are basically of two types: the junction field-effect transistor (JFET) and the insulated gate field-effect transistor (IGFET). The latter is more commonly known by a name metal-oxide semiconductor field-effect transistor (MOSFET).
At a point along the bar a region of p-type silicon forms a p-n junction. In normal operation, the junction is reverse-biased. The lower contact on the bar is called the source and the upper contact the drain. The electron current flows from source to drain and is controlled by the voltage applied to the p-region called the gate.
An alternative type of construction is the p-channel device where the gate is made of n-type material.
The operation of the JFET depends upon variations in the size of the depletion layer at the reverse-biased gate junction. The p-type gate is much more heavily doped than the n-type bar, so that the depletion region exists almost entirely in the bar. The gate carries a negative bias voltage relative to the source which give rise to the particular shape of the depletion region: this is wider at the top than the bottom. The wider the depletion layer, the narrower the channel there is available for the flow of electrons from source to drain, since the depletion region itself being devoid of current carries, behaves like an insulator.
Unlike the bipolar transistor, the FET employs only majority carriers for its operation. It is therefore sometimes called the unipolar transistor and is less susceptible than the bipolar type to temperature changes and nuclear radiation.
Пошаговое объяснение:
- щоб знайти дріб від числа, слід дріб помножити на це число
- щоб знайти відсоток від числа, слід виразити відсоток у вигляді десяткового дробу й помножити його на число
- щоб виразити відсоток у вигляді десяткового дробу, слід число відсотків поділити на сто
Тобто 60% = 0,6
3/5 = 0,6
Тому складемо й розв'яжемо рівняння:
3/5•0,6•x=72
0,6•0,6•х = 72
0,36х = 72
x = 72:0,36
x = 7200:36
x = 200
Для перевірки розв'язання знайдемо спочатку 60% від 200:
200:100*60=120
Тепер знайдемо 3/5 від 120:
120* 3/5= 24*3=72
Відповідь співпала з умовою.
Отож, х=200