6-5-4. Skillfully using capacitors
(1) Adjust the self-resonant frequency with the frequency of the
noise as a guide
The impedance of a capacitor is the minimum point of its
self-resonant frequency. This may be a smaller value than that of
the ideal capacitor at this frequency. If the frequency of the noise
is fixed, it is possible to obtain a significant noise reduction
effect, as long as the self-resonant frequency can be adjusted to
match the noise.
In order to adjust the self-resonant frequency, select a capacitor
with an electrostatic capacitance that matches the noise. As shown
in Figure 4, if the electrostatic capacitance of the capacitor is
changed, the characteristic curve where the capacitor is capacitive
moves in parallel. As shown in Fig. 16, the self-resonant frequency
also changes accordingly. The self-resonant frequency can thus be
adjusted to match the frequency of the noise.
However, the self resonant frequency is affected and changed by the
minute amount of inductance of the print board. This will be
explained later. The frequency cannot be adjusted well on paper, so
it is important to confirm the results during an actual test.
(2) If the noise frequency is wide, the only choice is to use a
capacitor with low ESL
When suppressing noise, it is generally difficult to estimate the
noise frequency ahead of time. In this case, a filter that works on
a wide range of frequencies must be prepared to ensure that the
filter is effective no matter what the noise frequency is. Method
(1) cannot be used for this kind of application.
Fig. 16 shows that the impedance in the area where the capacitor is
inductive (at 1GHz, for example) hardly changes at all even if the
electrostatic capacitance is changed. As explained earlier, this is
because ESL accounts for much of the capacitor's impedance at these
frequencies, and so it is difficult for electrostatic capacitance to
exert an effect.
The only way to suppress noise across a wide range of high
frequencies (at which the capacitor is inductive) is to use a
capacitor with as little ESL as possible.
(3) ESL may have an effect even on low frequency noise
In Fig. 13, ESL had an effect only at frequencies above 100MHz.
However, there may be cases where ESL exerts a strong effect even at
extremely low frequencies, when using a capacitor with a large
electrostatic capacitance. This is because the self-resonant
frequency is reduced, so the frequency range at which the capacitor
is inductive spreads to the lower frequencies.
Fig. 17 shows examples where the ESL was changed on a capacitor with
an electrostatic capacitance of 10μF. This shows that ESL can
exert a strong effect even at what are considered low frequencies
when it comes to noise suppression (such as 1MHz) . In cases like
this where the expected noise reduction effect cannot be obtained
with a large capacity capacitor, there is room to consider whether
or not ESL is exerting an effect.
Note however that the ESL of a bypass capacitor includes not only
the ESL of the capacitor itself, but the inductance of the wiring
used to install the parts. This will be explained in the next
section. Therefore, when attempting to reduce the ESL, it is also
important to consider the wiring used to install the capacitor.
(4) The pattern used to install the capacitor can be a factor behind
ESL
It was mentioned earlier that ESL has a significant effect on a
capacitor's noise reduction effect. However, there is one other
factor that plays a large role. This is the inductance generated
when installing the capacitor on a board.
As shown in Fig. 18, a wiring pattern and via are required to
install the capacitor to the board and connect it to the circuit.
The inductance of these parts is added in series to the bypass
capacitor. Therefore, when the capacitor is installed on a board and
actually operated, the overall ESL of the bypass circuit will be
greater than the ESL of the capacitor itself.
This "overall ESL" is what has an effect on the actual noise
reduction result.
(5) What is the effect of the pattern and via inductance?
What is the impact of the wiring and via inductance? It is actually
large enough that it cannot be ignored—in fact, the effect
might even be greater than that of the ESL of the capacitor itself,
depending on how it is being used.
Fig. 19 shows the results of calculating the impedance when a 1mm
wide pattern is installed on both ends of the capacitor. This shows
that even wiring that is only several mm wide can increase the
impedance at 100MHz ten times over or more.
When using a capacitor to reduce high frequency noise, the pattern
must be kept short.
(6) Approximate pattern and via inductance
How much ESL do patterns and via carry? The amount is extremely
small and cannot easily be measured or calculated. However, a
pattern will generally have around 0.5nH per 1mm, while a via will
generally have 0.1nH per unit. (Either case assumes comparatively
good conditions with a multi-layer board and a ground plane found
0.4mm below. The values will increase if using a double-sided board
or the like.)
Considering the fact that the ESL of the capacitor itself will be
around 0.5nH (even if an MLCC is used) , these values are large
enough that they cannot be ignored. The capacitor must be installed
in such a way that minimizes this inductance, if the capacitor is to
be used effectively.
(7) How to install capacitors to minimize ESL
Fig. 20 (b) and (c) show examples of installations where pattern and
via inductance are reduced.
Connect a ground plane or other solid ground to the capacitor. In
this figure, a board with a built-in ground plane is used.
Place the via that connects the capacitor and ground plane close to
the capacitor. If possible, arrange several vias around the
capacitor, as shown in the figure. Placing the via below the
capacitor will further reduce ESL.
Fig. 20 (b) shows an example where the capacitor is placed directly
over the wiring carrying the noise, with the wiring kept as short as
possible. Doing so will reduce the pattern and via inductance to a
level that can be ignored.
However, this method requires you to move the location of the via
connected to the ground.
Fig. 20 (c) shows an example of a solution for when the location of
the via cannot be moved. As shown in the figure, the capacitor is
placed close to the via connected to ground, while the pattern
carrying the noise is moved close to the capacitor. Doing this can
minimize the inductance in the direction noise is bypassed.
(8) Use a dedicated capacitor to eliminate noise exceeding 1GHz
The measurement results in Fig. 17 show that ESL must be around
0.2nH or less in order to obtain an impedance of 1 ohm or less at
1GHz. This value is so small that it would be impossible even with
an MLCC. You must also consider the inductance of the wiring and
via, as shown in Fig. 18. So how should it be installed?
A three-terminal capacitor ( (5) in Fig. 12) can be used to solve
this kind of problem. Capacitors with low ESL (such as
three-terminal capacitors) are used to suppress noise in frequencies
at 1GHz and higher. More details will be provided in Chapter 8.
Actual characteristics of capacitors" - Key
points
- Actual capacitors contain two types of parasitic elements:
ESL and ESR.
- The effect of parasitic elements is larger than the
electrostatic capacitance when eliminating noise at high
frequencies.
- Use capacitors with low ESL to eliminate a wide range of
noise above 100MHz.
- Note that ESL is also generated from the pattern used to
install the capacitor.