- Asked 9/28
- 2083 Baisakh · 7 marks
- 2081 Bhadra · 1+7 marks
- 2078 Bhadra · 2+6 marks
- 2075 Chaitra · 7 marks
- 2072 Chaitra · 6 marks
- 2069 Chaitra · 6 marks
- 2068 Chaitra · 2+6 marks
- 2071 Shrawan · 8 marks
- 2071 Chaitra · 8 marks
N-channel JFET construction and working
Short answer
An n-channel JFET has an n-type bar with p+ gate regions forming reverse-biased pn junctions. VGS controls depletion width and channel resistance. ID rises linearly with VDS then saturates at IDSS when VDS = |VP|. In saturation, ID = IDSS(1 – VGS/VP)².
Describe the construction and working principle of N-channel JFET with the help of characteristics curve and mathematical expressions.
A JFET (junction field-effect transistor) is a unipolar device in which the current flows through a channel of one doping type, controlled by the reverse bias on a gate p–n junction.
Construction (n-channel)
A bar of lightly doped n-type silicon forms the channel, with ohmic contacts at the ends: the drain (D) at the top and the source (S) at the bottom. Heavily doped p⁺ regions are diffused into both sides (and connected together) to form the gate (G). The p–n junctions create depletion regions that extend into the channel.
D
|
+----+-----+
| p+ n p+|
G --| channel |-- G
| p+ n p+|
+----+-----+
|
S
Working principle
- With VGS = 0 and a small positive VDS, electrons flow from source to drain through the channel; ID rises linearly with VDS (ohmic region), like a resistor.
- The gate junction is reverse biased (VGS ≤ 0). A more negative VGS widens the depletion regions, narrows the channel, increases its resistance and reduces ID. So VGS controls ID, like a voltage-controlled resistor/current source.
- For VGS = 0, as VDS increases, the reverse bias at the drain end is higher, so the depletion region is wider there. At VDS = |VP| (VP = pinch-off voltage) the channel pinches off near the drain, and ID saturates at IDSS (saturation current). Beyond that, ID remains almost constant (saturation/pinch-off region).
- At VGS = VP (negative, e.g. -4 V) the channel is completely closed: ID = 0 (cut-off).
- The gate current is almost zero (reverse-biased junction), so the input resistance is very high (10⁸ to 10¹⁰ Ω).
- Breakdown (avalanche) occurs at large VDS, beyond the saturation region.
Characteristics
Drain characteristics (ID vs VDS for different VGS):
ID
IDSS| _______ VGS = 0
| _-'
| / _______ VGS = -1 V
| / /
|/ / _______ VGS = -2 V
+--+------------ VDS
ohmic| saturation (breakdown)
Transfer characteristic (ID vs VGS) is a parabola from IDSS at VGS = 0 to zero at VGS = VP.
Drain current equation (Shockley)
In the saturation region:
ID = IDSS (1 - VGS/VP)² for VP ≤ VGS ≤ 0
where IDSS = drain current at VGS = 0 and VP = pinch-off voltage (negative for an n-channel JFET). Transconductance: gm = ∂ID/∂VGS = (2 IDSS/|VP|)(1 - VGS/VP) = gm0 (1 - VGS/VP), where gm0 = 2 IDSS/|VP|.
Condition for operating in the pinch-off (saturation) region: VDS ≥ VGS - VP (= VGS + |VP|).
✓ Answer checked by Claude Opus 5.5 (high effort)
Related questions
- JFET construction, curve and drain current equation · Electronics Devices and Circuit, chapter 3
- n-channel E-MOSFET construction and working · Electronics Devices and Circuit, chapter 3 · asked 9×
- D-MOSFET construction and working · Electronics Devices and Circuit, chapter 3 · asked 6×
- n-channel DMOSFET and JFET transconductance · Electronics Devices and Circuit, chapter 3
- EMOSFET principle, characteristics, ac model · Electronics Devices and Circuit, chapter 3
- Transconductance of BJT, JFET and MOSFET · Electronics Devices and Circuit, chapter 3
- N-channel enhancement MOSFET construction, working · Basic Electronics Engineering, chapter 3 · asked 9×
- N-channel depletion MOSFET construction, working · Basic Electronics Engineering, chapter 3 · asked 9×
- MOSFET construction and working principle · Basic Electronics Engineering, chapter 3 · asked 2×
- Rhombic antenna construction and working · Propagation and Antenna, chapter 3 · asked 5×