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Grounding The Essential Facts
By William D. Kimmel, P.E.
and Daryl D. Gerke, P.E.
We seem to write a lot about grounding probably because
we find so many problems there. The fact is that the overwhelming
number of EMI problems, whether emissions, immunity or self-compatibility,
have inadequate grounding at the root. That doesnt say
that you will solve your problems by grounding, but it does
say that good grounding is a necessary first step.
Grounding started before electronics was on the map
we grounded for lightning and electrical safety, which has
little to do with EMI. The early days of electronics was largely
the telephone people who discovered the single point ground
as a means of controlling low frequency interference to phone
lines. The radio people also learned about grounding, too,
but at high frequencies you wont see a single
point ground in the radio business.
Lets take a look at grounding its bare essentials.
We may not be able to solve your grounding problem, but we
can take a lot of the mystery out of it and at least steer
you in the right direction.
What Is A Ground?
In electronics, a ground is simply a current path. In most
cases, ground has no relationship with earth.
Earth ground has meaning only in the context of a lightning
strike to a surface structure. For our purposes, we can consider
ground to be a local reference for common circuits. We may
be more descriptive and add an adjective, as digital
ground, power ground, analog ground,
and so forth.
The Ground Loop
A ground loop exists whenever two or more circuits share
ground paths. Figure 1 shows the simplest case, that of two
circuits sharing a return path. All you need to know about
the effects of grounding is given by Ohms Law (substituting
impedance for resistance, as we are usually dealing with time-varying
signals):
V = IZ
We have indicated an impedance in the ground path to show
that there is always an impedance between two separate points.
Lets suppose that circuit A is a noisy circuit pulling
a significant amount of current, and that circuit B is a sensitive
high impedance circuit. The current drawn by circuit A will
drop a voltage Vn across the common return path. This noise
voltage shows up as an undesirable signal to the input of
circuit B.
The amount of noise voltage you can tolerate is application
specific. But once you decide how much Vn you can tolerate,
you are then left with two controllable variables, I and Z.
If either one can be reduced to zero, Vn is zero, and your
problems go away.
We cant get the common impedance to zero, but for many
cases, we can get close enough by using a ground plane which
is wide to lower inductive impedance.
Alas, we cant always get an adequately low impedance
ground, especially when we are dealing with systems level
grounding. In that case, we turn to the alternate variable
we reduce I to zero. Now thats an interesting
concept if we can reduce the current in circuit A to
zero, then the noise voltage drop across the ground impedance
becomes zero, and the problem is also solved. Unfortunately,
circuit A is there for a reason, and we have no control over
the current that it draws. But we dont have to reduce
the current to zero, we just have to reduce the current to
zero in the common return path, as shown in Figure 2. Here,
we see that the noisy circuit still exists and draws current,
but that current does not flow through the sensitive circuit
ground.
Note that you can ground the two circuits at one common point,
at either end (or anywhere in between, for that matter) without
compromising the solution, hence, the term single point
ground. This then is the essence of grounding: you can
either reduce the ground impedance to an acceptably low level,
or you can steer the ground currents along separate paths.
As a rule, you work with one or the other variable, but not
both.
Single Point Grounds
The single point ground is an elegant solution for sensitive
devices in low frequency applications. It is the holy grail
of telephones, sound systems and high impedance instrumentation.
It is particularly important in systems applications, where
cables may run for some distance, and where ground noise is
significant. A single point ground is usually desired for
power distribution, as well you want the return current
to come back on the wire, rather than on the enclosure or
structure.
That concept works well for these needs. Where doesnt
it work?
First, a single point ground assumes the speed of light is
infinite events in the paths of interest occur simultaneously.
For radio frequencies, that means that the distances must
be a small fraction of a wavelength anything longer
than that and you have the makings of an antenna. Note that
¼ wavelength is a worst case situation any ground
a ¼ wavelength long is an open circuit (we use 1/20
wavelength as an approximate boundary for the onset of distributed
behavior). For digital circuits, this includes any path length
a significant fraction of a risetime.
Second, a single point ground assumes that you have exactly
one ground path. This is achievable at audio frequencies,
but at higher frequencies field coupling paths become efficient
so that the ground currents dont necessarily follow
the designated conductive path. In short, single point grounds
dont exist at higher frequencies, no matter whether
they are desirable or not.
Note that you either have a single point or a multipoint ground
there is no such thing as almost a single point
ground. Once you have reached the point where a single
point ground is not achievable, you must use multipoint grounding
in your system.
Multipoint Ground
The most common case of a multipoint ground is on the printed
circuit board, especially the multilayer board the
ground plane provides a low impedance. In fact, for high speed
digital circuits, we need to use a ground plane in order to
keep the ground impedance low or the circuit wont work
at its intended speed. Our general rule of thumb is, if you
have a continuous ground plane, you are a good candidate for
multipoint grounds.
Once you leave the protection of a single enclosure, your
prospects for a multipoint ground diminish but do not become
impossible. If you have several enclosures in reasonably close
proximity (say, 10 feet), you can use a wide strap for a ground
plane. Our rule of thumb is to keep the length of the strap
no longer than five times the width. So a 10-foot-long ground
strap would need to be two feet wide.
If you find it impossible to achieve a single point ground,
your next best bet is to go to as many grounds as you can
to reduce ground impedance to a low value. For a systems application,
use ground grids and multiple ground straps.
Hybrid Grounds
Often, you need to have a single point ground for low level
low frequency signals and a multipoint ground for high frequencies
and high level signals and power. Then you turn to a hybrid
ground combining the best features of both.
One common hybrid is the frequency-dependent ground, most
commonly found in a cable shield, where one end is grounded,
the other end is terminated to ground through a small capacitor.
At low frequencies the capacitor looks like an open circuit,
providing the single point ground. At high frequencies the
capacitor looks like a short circuit, providing the multipoint
ground.
The second common hybrid segregates sensitive analog circuits,
noisy digital circuits and high level power circuits into
separate areas. Each area is a multipoint ground of similar
levels they are connected together in a common single
point ground. This provides a quiet area for the low level
analog circuits.
Summary
In most digital and RF applications, multipoint grounds
are necessary. This works well when you can keep the ground
impedances low, as would be provided by a ground plane. When
you cant get the ground impedance low enough, single
point grounds are appropriate. This would be more common in
systems applications, especially where low level analog signals
are present.
When deciding on your ground, start with Ohms Law. The
goal of a good ground is to reduce the noise voltage to an
acceptable level, either by reducing the impedance or by steering
the currents away from the affected path.
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