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AN9768 Datasheet, PDF (1/8 Pages) Littelfuse – Transient Suppression Devices and Principles
Transient Suppression Devices and Principles
Application Note
January 1998
AN9768
[ /Title
(AN97
68)
/Sub-
ject
(Tran-
sient
Sup-
pres-
sion
Device
s and
Princi-
ples)
/Autho
r ()
/Key-
words
(TVS,
Tran-
sient
Sup-
pres-
sion,
Protec-
tion,
High-
reli-
ability,
High
Reli-
ability,
Mil,
Transient Suppression Devices
There are two major categories of transient suppressors: a)
those that attenuate transients, thus preventing their
propagation into the sensitive circuit; and b) those that divert
transients away from sensitive loads and so limit the residual
voltages.
Attenuating a transient, that is, keeping it from propagating
away from its source or keeping it from impinging on a
sensitive load is accomplished with filters inserted in series
within a circuit. The filter, generally of the low-pass type,
attenuates the transient (high frequency) and allows the signal
or power flow (low-frequency) to continue undisturbed.
Diverting a transient can be accomplished with a
voltage-clamping type device or with a “crowbar” type
device. The designs of these two types, as well as their
operation and application, are different enough to warrant a
brief discussion of each in general terms. A more detailed
description will follow later in this section.
A voltage-clamping device is a component having a variable
impedance depending on the current flowing through the
device or on the voltage across its terminal. These devices
exhibit a nonlinear impedance characteristic that is, Ohm’s
law is applicable but the equation has a variable R. The
variation of the impedance is monotonic; in other words, it
does not contain discontinuities in contrast to the crowbar
device, which exhibits a turn-on action. The volt-ampere
characteristic of these clamping devices is somewhat
time-dependent, but they do not involve a time delay as do
the sparkover of a gap or the triggering of a thyristor.
With a voltage-clamping device, the circuit is essentially
unaffected by the presence of the device before and after the
transient for any steady-state voltage below the clamping
level. The voltage clamping action results from the increased
current drawn through the device as the voltage tends to
rise. If this current increase is greater than the voltage rise,
the impedance of the device is nonlinear (Figure 1). The
apparent “clamping” of the voltage results from the
increased voltage drop (IR) in the source impedance due to
the increased current. It should be clearly understood that
the device depends on the source impedance to produce the
clamping. One is seeing a voltage divider action at work,
where the ratio of the divider is not constant but changes.
However, if the source impedance is very low, then the ratio
is low. The suppressor cannot be effective with zero source
impedance (Figure 2) and works best when the voltage
divider action can be implemented.
1000
100
10
Z = 1Ω
NONLINEAR Z (α = 5)
Z = 10Ω
Z = 500Ω
IMPEDANCE
LINEAR
Z = 1Ω
1
0.01
0.1
1
10
100
CURRENT (A)
LINEAR IMPEDANCE: I =
V
R
NONLINEAR IMPEDANCE (POWER LAW): I = KVα
1000
FIGURE 1. VOLTAGE/CURRENT CHARACTERISTIC FOR A
LINEAR 1Ω RESISTOR AND NONLINEAR
ZS
VOC
ZV
VZV
=



Z----V----Z--+--V---Z----S--
VOC
FIGURE 2A. VOLTAGE CLAMPING DEVICE
ZS
Z1
VOC
R1
SCR
VZV
FIGURE 2B. CROWBAR DEVICE
FIGURE 2. DIVISION OF VOLTAGE WITH VARIABLE
IMPEDANCE SUPPRESSOR
10-102
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