MECHANISM OF
ELECTRONIC DEVICES
PRESENTED BY: MOUNTAIN MOVERS
MD. ASHRAFUL ISLAM TALUKDAR
MD. SHAKIL
RAKIB HOSSAIN
ABU KAISER MOHAMMAD MASUM
FOWJAEL AHAMED
N TYPE SEMICONDUCTOR
CENTRE TAP FULL WAVE RECTIFIER
Peak Inverse Voltage:
PIV=2𝑉𝑚
Disadvantages:
(i) Difficult to locate.
(ii) The dc output is small.
(iii) High peak inverse voltage
ZENER DIODE
What is Zener diode?
Equivalent circuit of a Zener diode
 Zener voltage
 Zener Resistance
Characteristics of a Zener diode
 Zener diode as voltage stabilizer
 Input voltage increases
 Load resistance decreases
FAITHFUL AMPLIFICATION
 Definition
 Basic conditions:
 Proper zero signal collector current
 Proper minimum base-emitter voltage (𝑉𝐵𝐸)
 Proper minimum collector-emitter voltage (𝑉𝐶𝐸)
Proper zero signal collector
current
Proper minimum base-emitter
voltage (𝑉𝐵𝐸)
Proper minimum collector-emitter
voltage (𝑉𝐶𝐸)
VOLTAGE DIVIDER BIAS METHOD
Circuit Analysis:
1. 𝐼𝑐
2. 𝑉𝐶𝐸
Collector Current IC:
I1 =VCC ̸ R1+ R2
So, voltage across resistance R2 is
V2 = (VCC ̸ R1+ R2) R2
Appling KVL to the base circuit of the Fig
V2 = VBE + VE
or, V2 = VBE + IERE
or, IE = (V2 - VBE) ̸ RE
Since, IE ≈ IC
∴ IC = (V2 - VBE) ̸ RE
Though IC depends upon VEE but in practice
V2 >> VBE, so that IC is practically
independent of VBE.
Collector-emitter voltage VCE:
Applying KVL to the collector side.
VCC = ICRC + VCE + IERE
= ICRC + VCE + ICRE [Because
IE = IC]
= IC (RC + RE) + VCE
VCE = VCC – IC (RC + RE)
Mechanism of Electronics Devices

Mechanism of Electronics Devices

  • 1.
    MECHANISM OF ELECTRONIC DEVICES PRESENTEDBY: MOUNTAIN MOVERS MD. ASHRAFUL ISLAM TALUKDAR MD. SHAKIL RAKIB HOSSAIN ABU KAISER MOHAMMAD MASUM FOWJAEL AHAMED
  • 2.
  • 3.
    CENTRE TAP FULLWAVE RECTIFIER Peak Inverse Voltage: PIV=2𝑉𝑚 Disadvantages: (i) Difficult to locate. (ii) The dc output is small. (iii) High peak inverse voltage
  • 4.
    ZENER DIODE What isZener diode? Equivalent circuit of a Zener diode  Zener voltage  Zener Resistance Characteristics of a Zener diode  Zener diode as voltage stabilizer  Input voltage increases  Load resistance decreases
  • 5.
    FAITHFUL AMPLIFICATION  Definition Basic conditions:  Proper zero signal collector current  Proper minimum base-emitter voltage (𝑉𝐵𝐸)  Proper minimum collector-emitter voltage (𝑉𝐶𝐸) Proper zero signal collector current Proper minimum base-emitter voltage (𝑉𝐵𝐸) Proper minimum collector-emitter voltage (𝑉𝐶𝐸)
  • 6.
    VOLTAGE DIVIDER BIASMETHOD Circuit Analysis: 1. 𝐼𝑐 2. 𝑉𝐶𝐸 Collector Current IC: I1 =VCC ̸ R1+ R2 So, voltage across resistance R2 is V2 = (VCC ̸ R1+ R2) R2 Appling KVL to the base circuit of the Fig V2 = VBE + VE or, V2 = VBE + IERE or, IE = (V2 - VBE) ̸ RE Since, IE ≈ IC ∴ IC = (V2 - VBE) ̸ RE Though IC depends upon VEE but in practice V2 >> VBE, so that IC is practically independent of VBE. Collector-emitter voltage VCE: Applying KVL to the collector side. VCC = ICRC + VCE + IERE = ICRC + VCE + ICRE [Because IE = IC] = IC (RC + RE) + VCE VCE = VCC – IC (RC + RE)