AN0005 RFMD | Alldatasheet
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Copyright 1997-2002 RF Micro Devices, Inc. Background Precompliance testing should be performed during the design process. This can be done with a GTEM cell or at a com- pliance test laboratory. It is recommended that precompliance testing be performed so that there are no surprises during final compliance testing. This will help keep the product development and release on schedule. Working with a laboratory offers the benefit of years of compliance testing experience and familiarity with the regulatory issues. Also, the laboratory can often provide feedback that will help the designer make the product compliant. On the other hand, having a GTEM cell or an open air test site locally offers the designer the ability to rapidly determine whether or not design changes impact the product's compliance. Set-up of an open air test site and the associated cali- bration is not trivial. An alternative is to use a GTEM test cell. After the design has been comp leted and passes compliance testing, final certifications will need to be obtained. Appli- cation will need to be made with the respective regulatory bodies for the geographi c region in which the product will be operated. Derivation of Conversion Factors In the Code of Federal Regulations Title 47, Part 15 there are numerous tables containing limits for emission levels. These limits are usually expressed as field strength in microvolts per meter at a given distance from the radiator. While one could use a field strength meter to measure the emissions of a device, such a test setup is not available in all labora- tories. However, most RF laboratories have spectrum analyzers. Thus, it would be desirable to establish a relationship between field strength and power. The following derivation is simplistic and makes the following assumptions:
- the emission is radiating isotropically
- the signal is being radiated into a sphere
- the power is being radiated evenly over the surface of that sphere
- the efficiency of the radiator is unity Represent the power density as Then the electric field, in microvolts per meter, can be represented as Now solve the equation to isolate transmitted power For the preceding equations the unit of power (P) is Watts, the unit of field strength (E) is microvolt per meter, the unit of distance (D) is meters. PDensity PTrans 4 π D2⋅⋅ E 11 0 6 377 PTrans⋅ 4 π D2⋅⋅ PTrans 4 π D2⋅⋅ 11 0 6⋅ 2 Converting Field Strength to Power AN0005 AN0005 Converting Field Strength to Power
Copyright 1997-2002 RF Micro Devices, Inc. To convert the power to decibels relative to a milliwatt (dBm), take the common (base 10) logarithm of the power and add thirty as below: Finally, this equation can be simplified to If the distance is three meters as is the case with many 47 CFR 15 specifications, the equation becomes Again, D is in meters and E is in µV/m. With this set of equations, one can convert between field strength and power. Below is a table containing some commonly encountered field strengths converted to power in dBm using the above equations. Field Strength Power 200µV/m @ 3m -49.20dBm 500µV/m @ 3m -41.25dBm 1250µV/m @ 3m -33.29dBm 12500µV/m @ 3m -13.29dBm 50mV/m @ 3m -1.25dBm PTrans dBm() 10 4 π D2⋅⋅ 11 0 6⋅ 2 ⋅log 30 +⋅= PTrans dBm() 20 DE ) 104.7713–⋅(log⋅= PTrans dBm() 20 E()log 95.2289–⋅=