Fairchild AN4148 Audible noise reduction technique Datasheet

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Application Note AN4148
Audible Noise Reduction Techniques for FPS
Applications
1. Introduction
- Capacitor Audible Noise
In general, switched mode power supplies do not generate
audible noise when they operate at constant ultrasonic
frequencies (>20kHz). However, some switched mode
power supplies can produce audible noise at certain load
conditions. Most Fairchild Power Switches are designed to
enter into burst switching operation at light load conditions
to reduce standby consumption, which can cause audible
noise when the fundamental frequency of the burst switching
bundles is in the range of human hearing as shown in Figure
1.
This application note explains the major sources of audible
noise and offers useful tips to engineers to solve the audible
noise problem in their Fairchild Power Switch (FPS)
applications.
Normal Switching Operation
3. Techniques to Reduce the Audible
Noise
- Varnish the Transformer
The most effective way to reduce the audible noise in the
transformer is to remove the possibility of physical
movement of the transformer elements by using adhesive
material or by varnishing. This damps mechanical resonance
of the transformer elements as well.
- Change the Transformer Design
above 20kHz
The amplitude of mechanical vibration of the transformer is
closely related to the flux swing. Therefore, the audible noise
can be reduced by lowering the flux swing in the burst
switching, which is given by
Burst Switching Operation
20~20kHz
Ceramic capacitors can also produce audible noise, since
they have piezoelectric characteristics. If there is still too
much audible noise in burst operation after gluing or
varnishing the transformer properly, the capacitor in the
snubber network should be examined.
above 20kHz
L I
Np Ae
6
m bp
- × 10
∆ B = --------------
(T)
(1)
Figure 1. Burst Switching Operation
2. Sources of Audible Noise
Even though the switching frequency of the FPS is above
the range of human hearing, audible noise can be generated
during transient or burst operation. In most flyback
converters, the major noise sources are transformers and
capacitors.
where Lm is the transformer primary side inductance, Ibp is
the current peak in burst switching, Ae is the cross-sectional
area of the core in mm2 and Np is the number of turns of
transformer primary side.
As can be observed in equation (1), the flux swing can be
reduced by increasing Np and/or Ae while keeping Lm
constant, which results in reduced audible noise.
- Reduce the Current Peak in Burst Switching
-Transformer Audible Noise
Transformers can produce audible noise, since they contain
many physically movable elements, such as coils, isolation
tapes and bobbins. The current in the coils produces electromagnetic fields which generate repulsive and/or attractive
forces between the coils. This can produce a mechanical
vibration in the coils, ferrite cores or isolation tapes.
Equation (1) also shows that the flux swing can be decreased
by reducing the current peak (Ibp) in burst switching. By
using slope compensation, the current peak in burst
switching can be reduced. Unfortunately, this technique can
be applied only to the FPSs below, whose burst switching
levels are determined by the feedback voltage level.
- FSDM0465R, FSDM0565R, FSDM07652R, FSDM1265R
- FSCM0565R, FSCM0765R, FSD200, FSD210
Rev. 1.0.0
©2005 Fairchild Semiconductor Corporation
AN4148
APPLICATION NOTE
The slope compensation circuit can be easily implemented
with one capacitor and one resistor as shown in Figure 2.
This slope compensation circuit introduces voltage dip in the
feedback voltage reducing the current peak in burst
switching as shown in Figures 3 and 4 with FSDM0565R as
an example. In the case of FSDM0565R, switching stops
when the feedback voltage drop below 0.5V and switching
resumes when the feedback voltage reaches 0.7V. Thus, the
burst switching current is determined by the feedback
voltage and can be reduced by introducing dip on the
feedback voltage.
V DC
R sn
+
V sn
+
C sn
Vo
-
D sn
FPS
Figure 4. Burst Switching Waveforms with Slope
Compensation (FSDM0565R)
Drain
GND
FB
- Change the RCD snubber network
Vcc
Na
817A
+
Ra
CB
47nF
Ca
Da
+
V SL
-
V FB
As mentioned in the previous session, ceramic capacitors
can also produce audible noise, because of their piezoelectric
characteristics. By replacing the ceramic capacitor with a
film capacitor as shown in Figure 5, the audible noise can be
reduced.
C SL
47nF
-
R SL
3k
Figure 2. Slope Compensation Circuit
Figure 5. Film Capacitor and Ceramic Capacitor
Figure 3. Burst Switching Waveforms without Slope
Compensation (FSDM0565R)
2
Another way to lower audible noise is to reduce the snubber
capacitor value, which decreases the pulse current that
charges the capacitor every time the FPS resumes switching
operation in burst mode as shown in Figure 6. A zener clamp
circuit using a TVS (Transient Voltage Suppressor) as shown
in Figure 7 can reduce the audible noise caused by the
snubber capacitor as well.
©2005 Fairchild Semiconductor Corporation
APPLICATION NOTE
AN4148
Vsn
Vdspeak
VDC
Vds
Vdspeak
- Change the Fundamental Frequency of Burst Switching
In general, human ears are most sensitive to frequencies of
2~4kHz and are less sensitive to frequencies which are
higher or lower as shown in the equal loudness curves of
Figure 8. These are graphical representations of the
sensitivity of the ear to frequencies over the range of human
hearing at various loudness levels. Each line shows the
intensity level for the range of frequency that gives a
subjective perception of similar loudness in reference to a
starting level at 1kHz.
Isn
Vds
Isn
Reducing the Snubber Capacitor
Figure 8. Equal Loudness Curves
Vds
Isn
Figure 6. Effect of Reducing the Snubber Capacitor
Rsn
Isn
Csn
FPS
TVS
(P6KE160CA)
Therefore, the subjective feeling of loudness can be lowered
by moving the fundamental frequency of noise out of the
2~4kHz range. The fundamental frequency of burst
switching can be changed by modifying the feedback
network. Figure 9 shows a typical feedback network. The
fundamental frequency can be reduced by one or more of the
following methods
- increasing CF
- increasing RD
- increasing CB
- decreasing RF
FPS
+
+
Vds
Vds
-
-
Figure 7. Zener Clamp Circuit with TVS
Figure 9. Typical Feedback Network of FPS
©2005 Fairchild Semiconductor Corporation
3
AN4148
APPLICATION NOTE
Figure 10 shows burst switching waveforms with feedback
network parameters as
- RF=1.2k, CF=100nF, RD=100, CB=22nF
In this case, the fundamental frequency of burst switching is
1.2kHz. When RD is increased from 100Ω to 1kΩ, the
fundamental frequency is reduced to 142Hz as shown in
Figure 11. With this circuit modification, the fundamental
frequency is lowered along with the subjective perception of
loudness. However, use caution when lowering the
fundamental frequency since the number of switchings in
each burst switching bundle as well as the output voltage
ripple increases when the fundamental frequency decreases.
Figure 10. Burst Switching Waveforms
(Fundamental Frequency is 1.2kHz)
Figure 11. Burst Switching Waveforms
(Fundamental Frequency is 142Hz)
4
©2005 Fairchild Semiconductor Corporation
AN4148
APPLICATION NOTE
by Hang-Seok Choi, Ph. D
Power Conversion Team / Fairchild Semiconductor
Phone : +82-32-680-1383 Facsimile : +82-32-680-1317
E-mail : [email protected]
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DOES IT CONVEY ANY LICENSE UNDER ITS PATENT RIGHTS, NOR THE RIGHTS OF OTHERS.
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