Electronics and Communication Engineering - Electromagnetic Field Theory
- Electromagnetic Field Theory - Section 1
- Electromagnetic Field Theory - Section 2
- Electromagnetic Field Theory - Section 3
- Electromagnetic Field Theory - Section 4
- Electromagnetic Field Theory - Section 5
- Electromagnetic Field Theory - Section 6
- Electromagnetic Field Theory - Section 7
- Electromagnetic Field Theory - Section 8
- Electromagnetic Field Theory - Section 9
- Electromagnetic Field Theory - Section 10
- Electromagnetic Field Theory - Section 11
- Electromagnetic Field Theory - Section 12
- Electromagnetic Field Theory - Section 13
- Electromagnetic Field Theory - Section 14
- Electromagnetic Field Theory - Section 15
- Electromagnetic Field Theory - Section 16
This is called field emission.
Therefore, conductivity increases.
Assertion (A): In a BJT, the base region is very thick.
Reason (R): In p-n-p transistor most of holes given off by emitter diffuse through the base.
Base region is thin.
Assertion (A): The behaviour of FET is similar to that of a pentode.
Reason (R): FETs and vacuum triode are voltage controlled devices.
Low work function permits easy emission.
- applying anode voltage at a sufficient fast rate
- applying sufficiently large anode voltage
- increasing the temperature of SCR to a sufficiently
- applying sufficiently large gate current.
If we apply the anode voltage above breakover voltage of SCR, SCR can be triggered. Also by sufficiently fast rate of rise of anode voltage and large gate current will trigger SCRon.
During forward blocking most of the applied voltage appears across reverse biased junction J2.
This voltage across J2 associated with leakage current may rise temperature of this junction.
With increase in temperature, leakage current through junction J2 further increases and this cumulative process may turn on the SCR at some high temperature.