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502R29W151KV3E-SC 参数 Datasheet PDF下载

502R29W151KV3E-SC图片预览
型号: 502R29W151KV3E-SC
PDF下载: 下载PDF文件 查看货源
内容描述: 辐射发射与iCoupler器件的控制建议 [Recommendations for Control of Radiated Emissions with iCoupler Devices]
分类和应用:
文件页数/大小: 20 页 / 645 K
品牌: ADI [ ADI ]
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Application Note  
AN-1109  
SOURCES OF RADIATED EMISSIONS  
There are two potential sources of emissions in PCBs: edge  
emissions and input-to-output dipole emissions.  
INPUT-TO-OUTPUT DIPOLE EMISSIONS  
The primary mechanism for radiation is an input-to-output  
dipole generated by driving a current source across a gap  
between ground planes. Isolators, by their very nature, drive  
current across gaps in ground planes. The inability of high  
frequency image charges associated with the transmitted cur-  
rent to return across the boundary causes differential signals  
across the gap driving the dipole. In some cases, this may be a  
large dipole, as shown in Figure 4. A similar mechanism causes  
high frequency signal lines to radiate when crossing splits in the  
ground and power planes. This type of radiation is predomi-  
nantly perpendicular to the ground planes.  
EDGE EMISSIONS  
Edge emissions occur when unintended currents meet the edges  
of ground and power planes. These unintended currents can  
originate from  
Ground and power noise, generated by inadequate bypass  
of high power current sinks.  
Cylindrically radiated magnetic fields coming from  
inductive via penetrations radiated out between board  
layers eventually meeting the board edge.  
Stripline image charge currents spreading from high  
frequency signal lines routed too close to the edge of  
the board.  
Edge emissions are generated where differential noise from  
many sources meet the edge of the board and leak out of a  
plane-to-plane space, acting as a wave guide (see Figure 2).  
GROUND  
POWER  
Figure 2. Edge Radiation from an Edge Matched Ground Power Pair  
GROUND  
POWER  
Figure 4. Dipole Radiation Between Input and Output  
h
The ADuM140x devices serve as a good example of the issues  
involved in generating and mitigating emissions.  
20h  
SIGNAL  
Figure 3. Edge Radiation from an Edge Mismatched Power Ground Pair  
When operating under a full 5 V VDD supply voltage, the peak  
currents of the transmitter pulses is about 70 mA, and these  
pulses are 1 ns wide with fast edge rates.  
At the edge boundary, there are two limiting conditions: the  
edges of the ground and power planes are aligned as in Figure 2  
or one edge is pulled back by some amount as shown in Figure 3.  
In the first case, with aligned edges, there is some reflection  
back into the PCB and some transmission of the fields out of  
the PCB. In the second case, the edges of the board make a  
structure similar to the edge of a patch antenna. When the  
edges mismatch by 20h where h is the plane-to-plane pacing,  
the fields efficiently couple out of the PCB, resulting in high  
emissions (see “Minimizing EMI Caused by Radially Propagating  
Waves Inside High Speed Digital Logic PCBs” in the References  
section). These two limiting cases are important considerations  
as described in the edge treatment of the PCB in the Edge  
Guarding section.  
Bypass capacitors are intended to provide this high frequency  
current locally. The capacitor must provide large charge reserves.  
At the same time, the capacitor should have a very low series  
resistance at high frequencies in the 100 MHz to 1 GHz range.  
Even with multiple low ESR capacitors near the pins, induc-  
tively limited bypassing generates voltage transients, and the  
noise may be injected onto the ground and power planes. The  
self-resonant frequency of capacitors should be considered.  
Having multiple capacitors of various sizes, 100 nF, 10 nF, and  
1 nF, may help reduce this effect.  
Figure 5 shows emissions data collected in an anechoic chamber  
taken with a 4-channel ADuM1402 with 5 V supplies, running  
at 1 Mbps signal frequency and using a standard 4-layer PCB,  
but without an input-to-output ground plane stitching  
capacitance.  
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