Recall-Lecture 7 - International Islamic University Malaysia
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Transcript Recall-Lecture 7 - International Islamic University Malaysia
Recall Lecture 8
• Standard Clipper Circuit
– Step 1: Find the clip value by doing KVL at the output
branch
– Step 2: Set the conditions to know whether diode is on or
off – sketch your output waveform
• Clipper in series
– clips at zero. It is similar to half wave where the diode only
turns on during one of the cycle.
Clamper
Clampers
● Clamping shifts the entire signal voltage
by a DC level.
Consider, the sinusoidal input voltage
signal, vI.
1st 900, the capacitor is charged up to
the peak value of VI which is VM.
Then, as VI moves towards the –ve
cycle,
the diode is reverse biased.
Ideally, capacitor cannot discharge,
hence Vc = VM
By KVL, we get
NOTE: The input signal is shifted by a dc
level; and that the peak-to-peak value is
the same
Clampers
●
A clamping circuit that includes an independent voltage source VB.
Peak value VM
STEP 1: Knowing what value that the capacitor is charged to. And from
the polarity of the diode, we know that it is charged during positive
cycle. Using KVL,
VC + VB – VS = 0 VC = VM – VB
STEP 2: When the diode is reversed biased and VC is already a constant
value
VO – VS + VC = 0 VO = VS – VC.
EXAMPLE – clampers with ideal diode
For the circuit shown in figure below, sketch the
waveforms of the output voltage, vout. The input voltage
is a sine wave where vin = 20 sin t. Assume ideal diodes.
Vin
What if the diode is non-ideal?
Vi
C
+
+
Vi
Vo
-
5V
The diode is a non-ideal
with V = 0.7V
-
10
t
-4.3
-10
-14.3
-24.3
Step 1: VC + V - VB – Vi = 0 VC = 10 + 5 – 0.7 = 14.3V
Step 2: VO – Vi + VC = 0 VO = Vi – 14.3.
Multiple Diode Circuits
Final Exam SEM I 2013/2014
DIODE
ID
VD
OFF
0
VD < V
ON
ID > 0
VD = V
REMEMBER THAT:
A pn junction diode will conduct when the p-type material is more
positive than the n-type material
OR GATE
Vo = voltage
across R
V1
V2
VO
D1 and D2 off; no current flow,
0
0
0
D1 off, D2 on, current flow,
Vo – V2 + V = 0
0
5V ( 1 )
4.3V
D1 on, D2 off, current flow,
Vo – V1 + V = 0
5V ( 1 )
0
4.3V
Both on, using both loops will
give the same equation
5V ( 1 )
5V ( 1 )
4.3V
AND GATE
Vo = node
voltage
V1
V2
VO
Both on, using both loops will
give the same equation
0
0
0.7
D1 on, D2 off
0
5V ( 1 )
0.7
D1 off, D2 on
5V ( 1 )
0
0.7V
Both are off; open circuit no
current flowing through R since
no GND destination
5V ( 1 )
5V ( 1 )
5V