Clipping and clamping diode circuits
Introduction
Certain
applications in electronics require that the upper or lower extremity of a wave
be fixed at a specific value. In such applications, a CLAMPING (or
CLAMPER) circuit is used. A clamping circuit clamps or restrains
either the upper or lower extremity of a waveform to a fixed dc potential. This
circuit is also known as a DIRECT-CURRENT RESTORER or a BASE-LINE
STABILIZER. Such circuits are used in test equipment, radar
systems, electronic countermeasure systems, and sonar systems. Depending upon
the equipment, you could find negative or positive clampers with or without
bias. Figure 4-16, views (A), illustrates some
examples of waveforms created by clampers. However, before we discuss
clampers, we will review some relevant points about series RC circuits.

Power
amplifiers, when driven out of their linear
range of operation, sound particularly bad, and can produce damage to
themselves or the transducers to which they are connected. The design of
traditional protection circuits is complicated by the various performance,
cost, and sonic tradeoffs involved. There is certainly no one right answer to
the limiter puzzle. The
circuits
presented here, however, are designed to maintain a high level of sonic
integrity, while remaining cost-effective.
These circuits
combine active limiting with a diode- based clipper to provide excellent driver
protection while avoiding the sonic degradation of simpler designs. An
innovative nonlinear capacitor circuit further improves the sonic performance
of the limiter.
a)
Limiters(clippers):
– Diodes can be used to clip off portions of signal voltages (above or
below
certain levels).

– Diode will become forward biased as soon as VA becomes larger than
VBIAS+0.7.
– When diode is forward biased, VA cannot
become larger than VBIAS + 0.7 V!
– Thus, the voltage across the load, RL, will
also be equal to VBIAS + 0.7.
– When diode is reverse biased, it appears as an open, so the output
voltage is
the voltage of RL alone.
- Desired voltage levels can be
attained with a voltage divider.

– We replace the voltage source with a resistive voltage divider.
VBIAS = R3/(R2 + R3)
VSUPPLY
b) Diode Clampers
– A clamper adds a dc level to an ac voltage.
– Also called dc restorers.
– When input voltage goes initially negative, diode is forward biased.
– Capacitor charges to near peak of inpt (Vp(in) – 0.7).
– Right after the negative peak, diode is reverse biased (because cathode
is held
near Vp(in)
– 0.7 by charge on capacitor).
– Capacitor can only discharge through the RL.
– Since RL
has high resistance, the
capacitor discharges very little each period.
– Note that time constant should be large (at least 10 times the period of
the
input voltage).
– Since capacitor retains charge, it acts like a battery in series with
the input
voltage.

Schottky Diodes
A concern in
many electronic systems
is the presence of
impulses of noise
or .voltage spikes. on
data or signal
lines. These undesired
transient signals can originate from within
or outside of
a given system,
and if severe enough,
can cause permanent damage to
system components such
as microprocessors. Long transmission
lines connecting different parts
of a system
are particularly susceptible to noise pickup
and are often the major culprits in noise and spike problems.
Clipping
and Clamping is the
deliberate limiting of a voltage at a circuit node or supply bus. Generally,
in the context
of using
Schottky
diodes for such
purposes, clipping is the
limiting of a
circuit node voltage
by using the forward
threshold voltage of a
diode. Clamping is the limiting of node voltage
in two directions
via use of
an anti- parallel pair
of clipping diodes.
In other words, clipping limits node
voltage below a certain
threshold; clamping limits node voltage within
a certain .window.
set by an anti-parallel diode
pair. The absolute
limiting voltage level(s) can be adjusted
by biasing the diode(s) with an
offset voltage via use of pull-up
or pull-down circuits.
Please refer to
Figure 1. Note that if the input signal voltage rises
above the supply voltage
due to .noise spikes., the upper diode will turn on,
dumping current into the VS node, limiting
the voltage at Node .A. to 1 diode drop above the supply voltage. Similarly,
if a negative-going transient on the data stream
dips more than 1 diode drop below ground, the lower diode will begin to
conduct, limiting Node .A. voltage to one
diode drop below
ground. In summary, the .window. of voltages allowed at
Node A is limited to a maximum of VS+VD, and a
minimum of .VD
(one diode drop
below
ground).
This assumes that
the diodes behave as perfect
switches. In reality, non- ideal diode
properties, including the
current- handling capability of the diode used, play a major
role in how well such clipping and clamping circuits
function in actual
practice. Note Figure 1. Diagram of a Clamping circuit using two Schottky
Diodes.
Desireable Characteristics of
Clipping /
Clamping Diodes,
or .Why Use
Schottky
Diodes?.
In
looking at the
circuit shown in Figure
1,
one can envision
several desired properties
for the diodes used:
1) Low
forward voltage
2) Fast
switching
3) High
current-handling capability

Use of the Clipping & Clamping Circuits
Basic Feedback Limiter with Diode
Clipper
The circuit shown in Figure 1 demonstrates the basic feedback limiter with adjustable clipper. The input signal is fed to the limiter circuitry at the node labeled “Input”. The limiter’s output is sent to the power amplifier from the point labeled “To Power Amplifier”. In addition, the output from the power amplifier is fed back to the limiter circuit by way of the node marked “From Power Amplifier Output”. Under normal operation, the input signal is below the limiter’s threshold and so the VCA is at unity gain, its lowest distortion region. For peak output levels of short duration which exceed the predetermined clip level, the clipper circuit “hard limits” the output to this level, performing very much like the (adjustable) diode clipper that it is. If the output level remains above threshold for long, the signal’s rms value will exceed the limiter’s average power threshold, causing the limiter to quickly reduce the level of signal being fed to the amplifier. In
this way, inaudible (but potentially damaging) peaks of short duration
will be clipped, while longer duration peaks will be handled by the limiter,
and little audible impairment should occur.

Figure 2 shows the clipper circuit used in this design. A
trans-impedance amplifier, OA3, converts the output current from the VCA
to a voltage which drives the actual clipper circuitry. When OA3’s output
voltage exceeds the threshold set by VR1, the transistor pair Q1
and Q2 combine to bypass R2 and clip the output to a fixed level. Using our
design example, the peak allowable power is specified as 220 VRMS,
and since we are ultimately clipping the signal to a square wave, this is
equivalent to 220 Vpeak. Given the power amplifier’s gain of 40, the
limiter must clip at 5.5 Vpeak. The two 1N4148 diodes prevent base-emitter
breakdown in Q1 and Q2. The addition of these diodes means that the clipping
voltage will be two diode drops (approximately 1.2 V) greater than the voltage
at the bases of Q1 and Q2. VR1 adjusts the voltage at the base of Q1 between 0
and -7.5 V, and at the base of Q2 between 0 and +7.5 V. Since we want the
limiter to clip at 5.5 V, VR1 should be adjusted to provide -4.3 V and 4.3 V at
the bases of Q1and Q2, respectively.

To form the limiter block, the VCA in Figure 1 is configured as a high-compression-ratio
feedback compressor. Under normal operation, the amplifier output is below the
compressor’s threshold voltage, the VCA’s EC- control port is kept
at zero volts, resulting in no compression or limiting action. Above the
threshold level, the threshold amplifier conducts and closes the feedback loop
from the RMS level-detector to the VCA, resulting in the desired limiter
function.
Advanced applications of
clipping & clamping circuits
DETAILED DESCRIPTION
The
GB4550(A) is intended for video applications requiring coarse DC restoration
coupled with flat frequency response. As shown in Figure 1, the signal path
features a wide band operational amplifier designed to be unity gain stable.
While this amplifer is not intended to drive 75 transmission lines,
it is
ideal for applications where high capactive loads, up to several hundred
picofarads, must be driven, such as input buffering and DC restoration of video
signals. Optimal frequency response for the GB4550(A) occurs with load capacitances
in the range of 80 pF to 100 pF as shown in Figure 4. For smaller loads, an
external capacitor can be added to extend the bandwidth and improve the
flatness of the device response. The clamping function is achieved through the
use of a simple comparator. The inverting input of the comparator is connected
to the GB4550(A) output, while the non-inverting input is connected to the
clamp voltage reference. For output signal voltages more positive than the
clamp reference the comparator output is essentially open-circuit, while signal
voltages more negative than the clamp reference result in the charging of CX. The action
of the comparator is to provide a positive current which is fed back to the
op-amp non-inverting input under conditions where the op-amp output is more
negative than the clamp reference voltage. This negative feedback raises the DC
level of the input signal to the point where all signal fluctuations occur at
voltages above the clamp reference level. This is the desired clamp action.
The input to the op-amp must be AC coupled using an appropriate size of
capacitor, which then acts as a DC "reservoir" for the corrective
level shift.
Under
equilibrium conditions the average current supplied by the comparator output is
just sufficient to balance the current discharging the input capacitor. This
discharge current is simply the input bias current of the op-amp, typically
less than 20 µA . However, an external resistor can be added to increase the
pull down current. Under dynamic conditions, where the system is adjusting for
a change in the signal level, the charging current may be in the milliamp
range. Because the corrective current is small under equilibrium conditions,
the error voltage at the comparator input is small also, so clamping accuracy
to within ±7 mV is achievable. The clamp circuit makes use of a "peak
hold" capacitor, CX, at the
output of the comparator . This gives rise to a more constant voltage at the
comparator output which is translated to a more constant corrective current by
an internal 100 k resistor
connected between the comparator output and the signal input.
To avoid
excessive phase shift and consequent instability of the clamp feedback loop,
the peak hold capacitor needs to be considerably smaller (e.g. 1000 times) than
the input coupling capacitor. If a faster clamp is desirable (e.g. for 60 Hz
hum elimination) the peak hold capacitor can be removed and a
smaller
input coupling capacitor employed. In this application some distortion of the
signal "tip" is unavoidable.



Conclusion
In my opinion , clipping and clamping circuits plays important rule in
electronics world , from protecting the delicate electronics circuits to
producing desired voltage signals , and much more applications beside
electronics