PQ48033QGA25NNS [SYNQOR]

DC-DC Regulated Power Supply Module, 1 Output, Hybrid, QUARTER BRICK PACKAGE-8;
PQ48033QGA25NNS
型号: PQ48033QGA25NNS
厂家: SYNQOR WORLDWIDE HEADQUARTERS    SYNQOR WORLDWIDE HEADQUARTERS
描述:

DC-DC Regulated Power Supply Module, 1 Output, Hybrid, QUARTER BRICK PACKAGE-8

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EMI Characteristics  
Application Note 00-08-02 Rev. 04 - 6/25/02  
Summary:  
This application note will give an overview of electromagnetic interfer-  
ence (EMI), the appropriate standards and regulations, how these stan-  
dards and regulations relate to dc/dc power modules, suggestions for  
external filtering solutions, and suggested layout and grounding prac-  
tices.  
1.0 Introduction  
Designing for electromagnetic compatibility (EMC) is one of the most difficult challenges for electronic system  
designers. Almost all-electronic equipment is required to meet one or more EMC standards at the system or  
product level. One of the most challenging subsystems when speaking about EMC is the power supply or in this  
case the dc/dc power module. All modern dc/dc converters are composed of one or more switching stages  
containing both pulsed voltages and currents, which generate a broad noise spectrum resulting in electromag-  
netic interference (EMI).  
This application note will give an overview of electromagnetic interference (EMI), the different standards and reg-  
ulations, how these standards and regulations relate to dc/dc power modules, suggestions for external filtering  
solutions, and suggested layout and grounding practices.  
The first step in designing systems for EMI compliance is to understand that the different standards and regula-  
tions do not directly apply to the dc/dc power module but to the overall system. Regardless, understanding and  
minimizing the emissions emanating from the power module is a good beginning to EMI system compliance.  
2.0 General Overview  
Electromagnetic interference (more commonly known as EMI) refers to how different sets of electronic equipment  
interact with each other, usually in a negative manner. The recent advances in semiconductor devices and large-  
scale integration has dramatically reduced the size of electronic equipment while increasing the probability for  
electromagnetic interference between the different systems and subsystems. Today's electronic designers must  
make sure their solutions work in an environment of high EMI. It is not practical to ask new product designers  
to test their equipment under all conditions and possible end-user configurations, therefore strict emissions regu-  
lations have been established. In the United States the Federal Communications Commission (FCC) regulates the  
use of radio and wire communications. Part of its responsibility concerns the control of electromagnetic inter-  
ference. The standards for the allowed levels of electromagnetic emissions are outlined in part 15 of the FCC  
rules and regulations. These rules apply to almost all-electronic equipment. Under these rules, limits are placed  
on the maximum allowable radiated emissions in the frequency range between 30 to 1000 MHz and on the  
maximum allowable conducted emissions on the AC power line in the frequency range of 0.450 to 30 MHz.  
Radiated Emissions  
Radiated emissions refer to interference that is coupled through the air. It is the belief of the FCC that at fre-  
quencies below 30 MHz the primary cause of EMI occurs by allowing RF to flow through the AC power lines  
where it subsequently radiates into neighboring equipment (conducted emissions).  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
All electronic equipment that generates pulses of any kind in excess of 10,000 pulses per second (> 10 kHz)  
is subjected to these regulations. Electronic equipment is divided into two classes according to the FCC:  
Class A: Electronic equipment that is marked for use in a commercial, industrial, or  
business environment [2].  
Class B: Electronic equipment that is marketed for use in a residential environment,  
notwithstanding its use in a commercial, industrial, or business environment [2].  
Class B equipment is more likely to be located in close proximity to radio and television receivers, therefore,  
the emissions limits for these devices is more restrictive relative to Class A. As it was stated before, compli-  
ance is the responsibility of the end-product manufacturer.  
Tables 1 and 2 show the different radiated emissions limits for both Class A and Class B. A true compari-  
son of these limits cannot be made unless they are compared at the same distance. The Class A limits can  
be extrapolated to a distance of 3-m by using a 1/r extrapolation where r is the distance between the source  
and the receiving equipment. In general, Class B limits are more restrictive by a factor of 3 (~ 10 dB) as  
shown in Figure 1.  
Measuring  
Distance (m)  
Field Strength  
(µV/m)  
Frequency  
(MHz)  
30 - 88  
88 - 216  
30  
30  
30  
30  
50  
70  
216 - 1000  
Table 1: FCC Class A Radiated Emmissions Limits [2].  
Measuring  
Distance (m)  
Field Strength  
(µV/m)  
Frequency  
(MHz)  
30 - 88  
88 - 216  
3
3
3
100  
150  
200  
216 - 1000  
Table 2: FCC Class B Radiated Emmissions Limits [2].  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
FCC Part 15, Subpart J radited emissions limits measured at  
a distanace of 3-m  
800  
700  
600  
500  
400  
300  
200  
100  
0
10  
100  
1000  
Frequency (MHz)  
Class B  
Class A  
Figure 1: Radiated emissions limits measured at a distance of 3.0m [1].  
Conducted Emissions  
Table 3 shows the conducted emission limits for both Class A and Class B type equipment. Conducted emissions  
are measured as the voltage measured common-mode (+Vin to ground and -Vin to ground) on the power line  
using a 50-ohm/50-µH line impedance stabilization network (LISN).  
Frequency  
(MHz)  
Class A  
Class B  
(µV)  
(µV)  
0.45 – 1.6  
1.6 - 30  
1000  
3000  
250  
250  
Table 3: FCC Conducted Emmission Limits [2].  
Standards  
The International Special Committee on Radio Interference (CISPR) regulates the international community. CISPR  
has no regulator authority, but its standards have been adopted by most European nations. Figure 2 shows a  
comparison between the CISPR recommended radiated emission standard and the FCC limits. The FCC limits  
have been scaled to a 10 m measuring distance for this comparison [1]. Figure 3 shows a similar comparison  
for the conducted emission standards. The limits in Figures 2 and 3 are displayed in decibels relative to 1 µV.  
The emission levels in decibels can be easily calculated using the following expression: emissions in decibels =  
20 log (noise level voltage/1µV).  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
FCC and CISPR Radiated Emission Limits  
50  
45  
40  
35  
30  
25  
10  
100  
1000  
Frequency (MHz)  
FCC Class A  
CISPR Class A  
FCC Class B  
CISPR Class B  
Figure 2: Radiated emission limits measured at a distance of 10 m [1].  
FCC and CISPR Conducted Emission Limits  
75  
70  
65  
60  
55  
50  
45  
40  
0.1  
1
10  
100  
Frequency (MHz)  
FCC Class A  
CISPR Class A  
FCC Class B  
CISPR Class B  
Figure 3: Conducted emission limits [1].  
FCC and CISPR also specify susceptibility emission limits of home electronics equipment and systems. To date,  
the FCC does not regulate the susceptibility of electronic equipment; the FCC relies on self-regulation by the  
industry. European nations are governed by the standards suggested by CISPR. Any product sold in Europe  
must meet these requirements. All SynQor power modules are tested and meet IEC PUBL. 1000-4-3 limits. IEC  
1000-4-3 test at field strengths of 3 V/m (normal performance) and 10 V/m (reduced performance). It has been  
shown that field strength greater than 2 V/m occurs for approximately 1 % of the time [1].  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
Another standard that is sometimes relevant is the EN300 386-2. This standard is relevant only for telecommu-  
nications equipment and it applies to equipment with either AC or DC power mains. For systems with DC input  
mains the EN300 386-2 standard specifies levels identical to the one specified by CISPR Class A limits.  
However, the EN300 386-2 standard extends to lower frequencies (20 kHz - 150 kHz). All of the SynQor  
power modules operate with switching frequencies in excess of 150 kHz. Therefore, typical power modules do  
not affect the low frequency emission levels of the system.  
3.0 EMC For Power Modules  
The first step in tackling the EMI problem is a thorough understanding of the requirements and how it relates to  
your system. Remember, there are no conducted or radiated emission restrictions that apply to power modules  
as a stand-alone product. Power modules are considered one of many components of modern telecom or com-  
puter equipment. The requirements apply to the system. The end product must meet a set of conducted and radi-  
ated emission levels that depends on the equipment usage and country into which it is being sold. Due to the  
fact that EMI is a system level requirement, it is not practical nor economical for high-power modules to meet  
either the conducted and radiated limits as a stand-alone component. Most high-power modules supplied by  
SynQor or any other manufacturer will probably not comply with the conducted and radiated limits specified by  
the different standards without some effort in the design of the system to limit noise.  
3.1 Conducted EMI  
Most electronic equipment has only one interface with the power source. It is at this interface that the conduct-  
ed emission standards apply. In most applications, power modules are usually isolated from the main power  
source by EMI filters, circuit breakers, fuses, transient protection devices, DC/DC converters, and/or AC/DC  
power converters. Therefore, in most applications the conducted emissions radiating from the power-module do  
not appear directly at the power mains. It is very possible that the system will meet the conducted EMI limits  
without any of the power modules meeting the EMC standard as a stand-alone component. Many systems will  
meet all EMI standards by simply using a single EMI filter at the input of the power mains.  
AC/DC and DC/DC converters by nature generate significant levels of both conducted and radiated noise.  
Furthermore, if these noises are not suppressed close to the source, they can very easily couple to other areas  
of the system, greatly  
increasing the complexity  
of  
the  
problem.  
Vd = V1 - V2 = differential mode voltage component  
Id = (I1 - I2) / 2 = differential mode current component  
Vc = (V1 + V2) / 2 = common mode voltage component  
Ic = I1 + I2 = common mode current component  
Cs = effective parasitic capacitance between the dc/dc/ module  
and the chassis ground  
Therefore, it is recom-  
mended to have some  
level of EMI suppression  
local to each power mod-  
ule.  
In order to better under-  
stand the source of con-  
ducted emissions, emis-  
sions are generally classi-  
fied as differential (sym-  
metrical) or common  
I1  
Id  
+
Ic/2  
Vd  
-
DC-DC  
Module  
I2  
Ic/2  
+
+
V1  
Id  
(asymmetrical)  
mode  
-
V2  
noise. The definition of  
common mode (CM) and  
differential mode (DM)  
voltages and currents is  
illustrated in Figure 3.  
Cs  
-
Ic  
Figure 3: Definition of differential and common mode currents and voltages.  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
The natural operation of dc/dc converters results in differential mode type currents and voltages. SynQor has  
added an input filter to all of its power modules to decrease the DM noise emitted by the converter. The com-  
mon mode noise emitted by the module cannot be directly determined since there is no direct coupling mecha-  
nism. The common mode current level is directly related to the effective parasitic capacitance between the power  
module and chassis ground. SynQor's power modules utilize an open frame design with no baseplate and no  
chassis ground connection. Not having a baseplate greatly reduces the effective capacitance between the mod-  
ule and chassis ground. Therefore, common mode currents are greatly reduced relative to typical power mod-  
ules.  
Figures 4 and 5 show a comparison of how the SynQor power modules differ from the traditional dc/dc mod-  
ule relative to their coupling mechanism for common mode emissions. Both of these figures present a simplified  
version of the common mode emissions problem in dc/dc modules. It is well known that there are many differ-  
ent coupling mechanisms between the power module and chassis ground. But at the same time as power sup-  
ply designers, we recognize that the semiconductor devices in conjunction with the power transformer represent  
the major sources of common mode voltages and currents. Figure 4 shows the traditional implementation of  
high-power dc/dc modules. Capacitance Cs1 represents the effective parasitic capacitance between the base-  
plate and chassis ground. Capacitance Cs1 is usually very small, its value is directly related to the size of the  
baseplate, the proximity of the baseplate to chassis ground, and the size and shape of the chassis ground. In  
many high-power modules the baseplate is directly connected to chassis ground shorting capacitance Cs1.  
Capacitance Cs2 is the parasitic capacitance between the semiconductor devices and the baseplate. In order  
to maximize the thermal performance of the module, in the traditional solution, a very thin thermal pad sepa-  
rates the "tab" of the semiconductor devices and the baseplate. This type of construction results in significant  
parasitic capacitance between the semiconductors and the baseplate. Capacitance Cs2 provides an easy cou-  
pling mechanism for common mode currents to flow into the chassis ground, especially when the baseplate is  
connected to chassis ground.  
Baseplate  
Cs1  
Baseplate  
Cs2  
Thermal Pad  
Semiconductor  
Devices  
Cs1 - parasitic capacitance between baseplate and chassis  
Cs2 - parasitic capacitance between semiconductor and baseplate  
Figure 4: Traditional physical design for high power dc/dc modules.  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
Figure 5 shows the physical solution of the SynQor power module. The preferred solution does not have a base-  
plate (Cs1 = 0). Capacitance Cs2 is the effective parasitic capacitance between the semiconductors and chas-  
sis ground. This capacitance is small relative to the traditional physical implementation, resulting in reduced  
common mode emissions.  
Semiconductor  
Devices  
Cs2  
FR4 Multilayer Board  
Integrated  
Magnetics  
Cs2 - parasitic capacitance between semiconductor(s) and chassis ground  
Figure 5: Physical design of a typical SynQor dc/dc module.  
SynQor offers a baseplate option on all of their modules (Figure 6). In this implementation, capacitance Cs2,  
which represents the effective capacitance between the semiconductor devices and the baseplate, again, is sig-  
nificantly smaller when compared to the traditional design. It is the proximity of the metal "tab" of the semi-  
conductor devices to the base plate that contributes to increased coupling (increased Cs2) and increased com-  
mon mode currents in the traditional arrangement. Therefore, SynQor's dc/dc power modules generate reduced  
levels of common mode emissions.  
Baseplate  
Semiconductor  
Devices  
Thermal  
Compound  
Cs1  
Baseplate  
Cs2  
FR4 Multilayer Board  
Integrated  
Magnetics  
Cs1 - parasitic capacitance between baseplate and chassis  
Cs2 - parasitic capacitance between semiconductor and baseplate  
Figure 6: Physical design of a SynQor module with the baseplate option.  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
Table 4 summarizes the EMC related characteristics of selected SynQor modules. Please consult the individual  
datasheet for specific data on each module. The switching frequency is listed to help understand the noise spec-  
trum and help in the design of an external filter. It is important to note that the switching frequency of the mod-  
ules has a tolerance of +/- 17 % over temperature. The table summarizes the characteristics of the input filter.  
Most modules have a Pi type filter at the input. C1 is the capacitance connected directly at the input pins. C2  
is the second capacitor of the Pi filter. In all of the SynQor modules, the inductor is located in the +Vin lead.  
Nominal  
Input  
Capacitance  
C1, C2 (µF)  
Input  
Inductor  
(µH)  
Operating  
Frequency  
(kHz)  
Module Type  
Input Filter  
PQ48150QGA06NNS  
PQ48120QGA08NNS  
PQ48060QGA17NNS  
PQ48050QGA20NNS  
PQ48033QGA25NNS  
PQ48025QGA25NNS  
PQ48020QGA25NNS  
PQ48018QGA25NNS  
PQ48015QGA25NNS  
PQ48050HTA33NNS  
PQ48033HTA50NNS  
PQ48025HTA60NNS  
PQ48020HTA60NNS  
PQ48018HTA60NNS  
PQ48015HTA60NNS  
270  
215  
215  
300  
240  
200  
270  
240  
200  
200  
260  
200  
200  
200  
260  
2nd order  
2nd order  
2nd order  
2nd order  
2nd order  
2nd order  
2nd order  
2nd order  
2nd order  
Pi  
0, 2.46  
0, 2.46  
4.7  
4.7  
4.7  
4.7  
4.7  
4.7  
4.7  
4.7  
4.7  
4.1  
4.1  
4.1  
4.1  
4.1  
4.1  
0, 2.46  
0, 2.46  
0, 2.46  
0, 2.46  
0, 2.46  
0, 2.46  
0, 2.46  
1.64, 3.28  
1.64, 3.28  
1.64, 3.28  
1.64, 3.28  
1.64, 3.28  
1.64, 3.28  
Pi  
Pi  
Pi  
Pi  
Pi  
Table 4: EMC characteristics of the SynQor power modules. Refer to individual technical  
datasheets for information on specific modules.  
Figures 7, and 8 show the conducted emissions of the 25A quarter-brick and the 50A half-brick 3.3V modules  
operating at full load with the aid of an external filter. The modules were tested in an independent Lab (KTL of  
Dallas) in accordance with the accepted CISPR standards. The modules were loaded with a passive resistive  
load to avoid any possible interaction between the "dynamic load" and the module. The units were mounted  
on a four layer test board where the bottom layer was used for a chassis ground plane. The results show peak  
measurements relative to the average Class B (CISPR) limits. The implementation of the two external filters used  
is summarized in Figure 9. The suggested filters allow for the modules to meet CISPR Class B conducted emis-  
sions limits. Capacitors CYS1 and CYS2 are added to minimize the electromagnetic interference emanating  
from the output cables in the 5 to 30 MHz frequency range. These capacitors could be omitted if the output dis-  
tribution bus is relatively short in length.  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
Figure 7a: Conducted emission from 150 kHz to 600 kHz for the 25A quarter-brick using the  
EMI filter shown in Figure 9a [6]. The data shown corresponds to the emission meas-  
ured in the positive input lead. The 50-dBµV level is shown as a reference.  
Figure 7b: Conducted emission from 500 kHz to 30 MHz for the 25A quarter-brick using the  
EMI filter shown in Figure 9a [6]. The data shown corresponds to the emission meas-  
ured in the positive input lead. The 50-dBµV level is shown as a reference.  
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EMI Characteristics  
Figure 8a: Conducted emission from 150 kHz to 600 kHz for the 50A half-brick using the EMI  
filter shown in Figure 9b [6]. The data shown corresponds to the emission measured  
in the positive input lead. The 60-dBµV level is shown as a reference.  
Figure 8b: Conducted emission from 500 kHz to 30 MHz for the 50A half-brick using the EMI  
filter shown in Figure 9b [6]. The data shown corresponds to the emission measured  
in the positive input lead. The 60-dBµV level is shown as a reference.  
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EMI Characteristics  
Filter Mod. # 4  
CYS2  
CY2  
PQ48033QGA25NNS  
DC/DC Converter  
C
CD2  
CD1  
L1  
E
Rload  
CY1  
CYS1  
CY1 = CY2 = CYS1 =CYS2 = 2700 pF /2000V ceramic capacitor from AVX  
CD1 = CD2 = 3 x 1µF /100V ceramic capacitor from AVX  
L1 = inductor (Pulse part# P0422)  
C = 33µF /100V electrolytic capacitor, Refer to “Input System Instability” application note for details.  
E
Iout = 25 Amps  
Figure 9a: External filter used with the PQ48033QGA25NNS (quarter-brick 25A/3.3V)  
power module.  
Filter Mod. # 5  
CYS2  
CYS1  
CY2  
CY1  
CD1  
L1  
PQ48033HTA50NNS  
DC/DC Converter  
CD3  
Rload  
L2  
CD2  
C
E
CY1 = CY2 = CYS1 =CYS2 = 2700 pF /2000V ceramic capacitor from AVX  
CD1 = CD2 = CD3 = 2 x 1µF /100V ceramic capacitor from AVX  
L1 = inductor (Pulse part# P0353)  
C = 33µF /100V electrolytic capacitor  
E
Iout = 50 Amps  
Figure 9b: External filter used with the PQ48033HTA50NNS (half-brick 50A/3.3V)  
power module.  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
3.2 Radiated EMI  
Again it is important to remember that only the system needs to meet the required standards. Radiated emis-  
sions are of importance in the 30 MHz to 1000 MHz range. Metal enclosures in addition to power and ground  
planes provide significant attenuation to electromagnetic emissions in the frequency range in question.  
Therefore, most physical system solutions will provide enough attenuation and allow the system to meet radiat-  
ed emission standards with relative ease. It is neither practical nor economical to demand the typical dc/dc  
module to meet radiated EMC standards as a stand-alone product.  
A one-piece metal "box" with no opening or cracks would be the ideal shield to radiated noise, but this is not  
a practical solution. When designing for radiated emissions it is important to minimize the size of any opening  
in the chassis box. The size of any opening in addition to its location relative to the source of radiated EMI is  
of great importance as it concerns radiated EMI. Furthermore, any location where two or more metal pieces of  
the chassis box meet needs to make electrical contact to maintain the integrity of the shield.  
Again, radiated emissions are classified into differential and common mode depending on the source.  
Differential-mode noise radiates from small loop antennas. Loop antennas can be defined as the area enclosed  
by a current carrying loop. The magnitude of the field is proportional to the magnitude of the current, the  
enclosed area, and the square of the oscillating frequency. Reducing the area enclosed by any current loop can  
easily minimize differential-mode noise. Great care has been taken in the layout of all SynQor power modules  
to reduce differential mode radiation.  
On the other hand, common-mode radiation is harder to control and usually determines the overall radiated emis-  
sion performance of the product. Common-mode radiation usually emanates from the input and output cables.  
Due to their relatively long length, input and output mains are good transmitters of EMI noise. Input and output  
cables behave as monopole antennas driven by a voltage. Decoupling both input and output mains with ceram-  
ic capacitors to chassis ground close to the power module suppresses the excitation voltage. Great care has to  
be taken not to exceed the leakage current requirement (this is a safety requirement) when adding capacitors  
from any point to chassis ground in systems powered by an AC distribution.  
For reference, Table 5 shows radiated emissions levels for a 25A quarter-brick 3.3Vout module operating at full  
load. The module was tested with the external filter suggested in Figure 9a in place. Again, a resistive load  
bank was used to obtain these results. The tables show peak measurements of the radiated emissions levels rel-  
ative to the average Class B limits as suggested by CISPR. The data shows that the module and filter combina-  
tion fails CISPR Class B emissions standards by only a few dBs. The module was tested in an outdoor inde-  
pendent test facility at KTL of Dallas.  
The conducted and radiated emissions levels reported for the different modules should be used as a reference  
only. The emissions levels are very dependent on the physical configuration and grounding practices of the sys-  
tem under test.  
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Application Note 00-08-02 Rev. 04  
EMI Characteristics  
Antenna  
Polarization (dBµV/m)  
Reading  
Class B limit  
(dBµV/m)  
Diff.  
(dB)  
Type of  
Measurement  
Frequency  
(MHz)  
30.17  
30.66  
36.20  
37.71  
48.76  
H
H
H
H
H
H
H
H
H
H
H
H
H
H
H
30.9  
1.929.7  
1.637.1  
37.8  
28.7  
31.2  
23.4  
27.5  
43.5  
43.5  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
0.9  
-0.3  
7.1  
7.8  
-1.3  
1.2  
-6.6  
-2.5  
13.5  
13.5  
2.8  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
52.03  
86.46  
108.80  
141.28  
142.80  
160.38  
165.13  
208.90  
221.90  
228.48  
32.8  
32.5  
29.2  
27.4  
2.5  
-0.8  
-2.6  
-1.9  
28.1  
36.20  
36.20  
37.75  
37.75  
50.30  
50.30  
52.03  
62.84  
74.60  
V
V
V
V
V
V
V
V
V
V
V
V
V
V
V
V
V
V
V
48.2  
32.4  
48.0  
32.4  
40.5  
25.5  
36.3  
33.8  
28.2  
31.1  
35.5  
36.1  
41.8  
32.3  
42.4  
32.4  
30.1  
28.1  
26.3  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
30.0  
18.2  
2.4  
18.0  
2.4  
10.5  
-4.4  
6.3  
3.8  
-1.8  
1.1  
5.5  
6.1  
11.8  
2.3  
12.4  
2.4  
0.1  
-1.9  
-3.7  
Peak  
Quasi-Peak  
Peak  
Quasi-Peak  
Peak  
Quasi-Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
Peak  
85.96  
119.13  
125.40  
142.50  
142.50  
144.00  
144.00  
165.10  
208.80  
224.90  
Quasi-Peak  
Peak  
Quasi-Peak  
Peak  
Peak  
Peak  
302.57  
343.57  
377.50  
H
H
H
26.0  
27.8  
25.1  
37.0  
37.0  
37.0  
-11.0  
-9.2  
-11.9  
Peak  
Peak  
Peak  
301.87  
334.08  
438.00  
V
V
V
23.0  
19.9  
22.6  
37.0  
37.0  
37.0  
-14.0  
-17.1  
-14.4  
Peak  
Peak  
Peak  
Table 5: Radiated emissions of a 25A Quarter-brick 3.3V module with the external filter  
shown in Figure 9a.  
Page 13  
SynQor - Advancing the Power Curve  
888-567-9596 www.synqor.com  
Application Note 00-08-02 Rev. 04  
EMI Characteristics  
4.0 Layout and Grounding Practices  
Great care should be taken in the layout and grounding practices used for the module and system in general.  
A list of suggestions that will minimize conducted and radiated emissions include:  
1. Add both, low frequency tantalum and high frequency ceramic capacitors to the dc/dc  
module output bus. Place at least one of each as close as possible to the output termi-  
nals of the module.  
2. Add both, low frequency electrolytic and high frequency ceramic capacitor to the dc  
input distribution bus. Place at least one of each as close as possible to the input ter-  
minals of the module.  
3. Use short leads on all filter and decoupling components. Minimize all circuit loops that  
carry significant current.  
4. Minimize parasitic inductances by using wide distribution traces over ground planes.  
5. Place a Y-capacitor between input and output ground planes. Return all common mode  
noise to the input ground.  
Additional details about all of these topics can be found in [1,4].  
5.0 References  
[1] Ott, Henry, W., Noise Reduction Techniques in Electronic Systems, Second Edition, John Wiley & Sons, New  
York, 1988.  
[2] Code of Federal Regulations, Title 47 (47CFR). Part 15, Subpart J. "Computing Devices."  
[3] CISPR, Publication 22. "Limits and Methods of Measurements of Radio Interference Characteristics of  
Information Technology Equipment," 1985.  
[4] Thihanyi, Laszlo, Electromagnetic Compatibility in Power Electronics, 10th edition, J. K. Eckert & Company,  
Inc., Sarasota, Florida, 1995.  
[5] Ferreira, J.A., Winlock, P.R., and Holm, S.R., "Sources, Paths and Traps of Conducted EMI in Switch Mode  
Circuits,"  
[6] KTL Engineering test report # 0L0073EUS  
155 Swanson Rd., Boxboro, MA 01719  
Phone: 978-849-0600  
Toll Free: 888-567-9596  
Fax: 978-849-0602  
Web: www.synqor.com  
e-mail: sales@synqor.com  
Author: Richard Farrington  
Page 14  
SynQor - Advancing the Power Curve  
888-567-9596 www.synqor.com  

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