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Ferrite
Bead
Introduction
 A ferrite bead is a passive device that filters high
frequency noise energy over a broad frequency range.
It becomes resistive over its intended frequency range
and dissipates the noise energy in the form of heat.
 The ferrite bead is connected in series with the power
supply rail and is often combined with capacitors to
ground on either side of the bead.
This forms a low-pass filter network,
further reducing the high frequency
power supply noise[1].
2
Introduction
 Ferrite beads are categorized by three response regions:
inductive, resistive, and capacitive. To reduce high
frequency noise, the bead must be in the resistive
region, and it acts like a resistor[1].
 The inductive region occurs
below the bead crossover
frequency (X = R),
where the bead becomes
inductive and acts like
a inductor[1].
3
Unwanted resonance
 Nevertheless, improper combining ferrite beads with a
decoupling capacitor for low-pass filtering can lead to
unwanted resonance below the bead crossover
frequency (X = R).
 Unwanted resonance may amplify ripple and noise in a
given system instead of attenuating it[1].
V+
V-
Ferrite bead, but
acts like a
inductor
Series Resonance
Decoupling
Capacitor
 Unwanted resonance frequencies for typical bead filters
are generally in the 0.1 MHz to 10 MHz range.
For typical switching frequencies
in the 300 kHz to 5 MHz range[1].
4
Unwanted resonance
 For example, the ferrite bead used is a TDK
MPZ1608S101A (100 Ω, 3 A, 0603) and the decoupling
capacitor used is a Murata GRM188R71H103KA01 low
ESR ceramic capacitor (10 nF, X7R, 0603).
5
Unwanted resonance
 Apparently, unwanted resonance occurs at ~2.5 MHz
due to (bead-C) combination, which forms series
resonance mechanism.
 As mentioned earlier,
this unwanted resonance
may amplify
ripple and noise.
6
Unwanted resonance and IR Drop
 Thus, (bead+C) combination makes PA power supply
unstable and ACLR aggravates.
 In addition, the ferrite bead’s large DCR may lead to
large IR drop, which aggravates ACLR as well,
especially at maximum RF output power because
current is large.
PA
Bead
IR Drop = I*DCR
7
How to solve this problem ?
 In terms of DCR, we ought to choose a ferrite bead with
small DCR.
 In terms of unwanted resonance, using an additional
RC decoupling filter can reduce the unwanted
resonance[1].
8
Reference
[1] Ferrite Beads Demystified, Analog Devices
9

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Why Ferrite Beads Aggravates ACLR

  • 1. 1
  • 2. Ferrite Bead Introduction  A ferrite bead is a passive device that filters high frequency noise energy over a broad frequency range. It becomes resistive over its intended frequency range and dissipates the noise energy in the form of heat.  The ferrite bead is connected in series with the power supply rail and is often combined with capacitors to ground on either side of the bead. This forms a low-pass filter network, further reducing the high frequency power supply noise[1]. 2
  • 3. Introduction  Ferrite beads are categorized by three response regions: inductive, resistive, and capacitive. To reduce high frequency noise, the bead must be in the resistive region, and it acts like a resistor[1].  The inductive region occurs below the bead crossover frequency (X = R), where the bead becomes inductive and acts like a inductor[1]. 3
  • 4. Unwanted resonance  Nevertheless, improper combining ferrite beads with a decoupling capacitor for low-pass filtering can lead to unwanted resonance below the bead crossover frequency (X = R).  Unwanted resonance may amplify ripple and noise in a given system instead of attenuating it[1]. V+ V- Ferrite bead, but acts like a inductor Series Resonance Decoupling Capacitor  Unwanted resonance frequencies for typical bead filters are generally in the 0.1 MHz to 10 MHz range. For typical switching frequencies in the 300 kHz to 5 MHz range[1]. 4
  • 5. Unwanted resonance  For example, the ferrite bead used is a TDK MPZ1608S101A (100 Ω, 3 A, 0603) and the decoupling capacitor used is a Murata GRM188R71H103KA01 low ESR ceramic capacitor (10 nF, X7R, 0603). 5
  • 6. Unwanted resonance  Apparently, unwanted resonance occurs at ~2.5 MHz due to (bead-C) combination, which forms series resonance mechanism.  As mentioned earlier, this unwanted resonance may amplify ripple and noise. 6
  • 7. Unwanted resonance and IR Drop  Thus, (bead+C) combination makes PA power supply unstable and ACLR aggravates.  In addition, the ferrite bead’s large DCR may lead to large IR drop, which aggravates ACLR as well, especially at maximum RF output power because current is large. PA Bead IR Drop = I*DCR 7
  • 8. How to solve this problem ?  In terms of DCR, we ought to choose a ferrite bead with small DCR.  In terms of unwanted resonance, using an additional RC decoupling filter can reduce the unwanted resonance[1]. 8
  • 9. Reference [1] Ferrite Beads Demystified, Analog Devices 9