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PL75-9 Datasheet(PDF) 82 Page - List of Unclassifed Manufacturers |
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PL75-9 Datasheet(HTML) 82 Page - List of Unclassifed Manufacturers |
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82 / 141 page ![]() R Trompeter Products Catalog - T21 Military/Aerospace ISO 9001 Registered (800) 982-2629 Fax: (818) 706-1040 www.trompeter.com 82 signal transmission in high frequency/high density applications Impedance An inherent characteristic for transmission lines is impedance, which is measured in ohms. Impedance is the ratio of voltage to current in a traveling wave. For a "loss-less" cable, it can be defined in terms of the ratio of inductance to capacitance. In a coaxial construction, it can be alternatively defined as a function of geometry and material properties of the dielectric material between the concentric conductors. This equation can be stated as : Z 0 = character impedance ε = dielectric constant of the insulation material D = inside diameter of the outer conductor d = outside diameter of the inner conductor Physically, impedance can be thought of as the value of resis- tance that, when connected between the center conductor and shield at the end of the cable, makes the cable appear infinitely long. The most efficient transmission of electrical power, hence maximum signal transfer, occurs when the distributed compo- nent impedance matches that of the system. Impedance mismatch creates a reflected wave of energy, which can be measured and stated in different forms. By defining a reflection coefficient ( ρ), which is the reflected voltage divided by incident voltage, the measure of reflection losses can be stated as: Reflection Loss (dB) = 10 Log 10 (1 / 1-ρ 2) dB or Voltage Standing Wave Ratio (VSWR) = (1+ρ) / (1-ρ) Return loss is the decibel loss due to reflection, and VSWR is a unitless ratio relating incident voltage to reflected voltage. These commonly used terms that quantify the loss associated with reflection are two scales for the same characteristic. They can be equated as follows: Return Loss (dB) = 20 Log 10 {(VSWR + 1) / (VSWR -1)} Reflection losses are a function of frequency - increasing with increasing frequency - and impedance mismatch. It is helpful to note that VSWR is the ratio of the maximum standing wave voltage to the minimum standing wave voltage. VSWR, there- fore, is infinite for total reflection (i.e. 0 minimum voltage) and is 1.0 for perfect transmission (no reflection). The closer to unity, the better the impedance match and the more efficient the transmission system. Three Examples Figure 1 (on page 81) shows comparison return loss data from 1 MHz through 2 GHz for the following three scenarios: 1. 75 Ω system (includes cable and test set); 50Ω BNC connector; 2. 75 Ω system; approximate 75Ω BNC connector; and 3. 75 Ω system; "true" 75Ω BNC connector. From this, it is clear that the return loss degrades as a function of the frequency and also as a function of the extent of the impedance mismatch between the connector and cable. At higher frequencies the impedance match becomes more critical. Other factors influence the reflection loss as well. These include: the homogeneity of a composite dielectric material; the even dispersion of air within and around a dielectric; and the "smoothing" of the mechanical transmissions between the im- pedance mismatches within the connector. This includes the tandem increase or decrease in sizing of the diameters for the inner and outer conductor, as well as the effect of chamfers/ breaks at sharp transitions. Other Considerations Aside from the electrical and electromagnetic performance issues, connectors that disconnect should be capable of tough- ness, durability and robust in-field use with high counts of repeat mating cycles without failure or interruption. Other nonelectri- cal performance measures of importance are insertion force and retention force, particularly after repeated matings. Conclusion Market Trends, Technical Considerations and Practical Examples for Shielded Disconnectable Interconnects Market needs are impacting electrical and electromagnetic de- mands on connector performance. A basic understanding of the physics involved in electrical circuit design and transition lines is necessary to appreciate the impact of losses associated with the connector. This understanding includes resistance, capaci- tance, inductance, efficiency, reflection losses associated with impedance mismatch, and dielectric losses associated with the materials used for connector dielectrics. Impedance mismatch between the source, cable and connector is less significant at lower than at higher frequencies. However, as system content and speed increases, the permissible fault tolerances goes down dramatically. In other words, one impact of high technology is greater dependance on tighter tolerance quality and part-to-part repeatability. These discoveries have caused shifts in sourcing, as buying companies mature in their appreciation for robust design engineering and fabrication ex- cellence. The connector industry is not immune from this development. ■ Z 0 138 = √ε (Log D/d) 10 |
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