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ing, usually due to rubbing contacts between their shoes or clothing and dissimilar materials used for flooring, storage, and the like. General Information. Equipment, systems, subsystems, and peripherals may be involved in static electricity discharges due to environmental and installation conditions. These conditions include low relative humidity, use of lowconductivity (artificial-fiber) carpets, vinyl garments, and the like. Generation of electrostatic charges is favored by the combination of various fabrics and a dry atmosphere. There are many variations in the charging process. A common situation is one where a person walks on carpet. With each step, the person loses or gains electrons from the body to the fabric. Friction between the person s clothing and a chair can also produce an exchange of charge, often in the thousandsof-volts range. A conducting carpet provides no protection unless the operator is adequately earthed to it. Equipment may be directly subjected to discharges of voltage up to several kilovolts, depending on the type of synthetic fabric and the relative humidity of the environment. Energy transfer is a function of the discharge current rather than the electrostatic voltage that exists prior to the discharge. Discharge current is typically less than proportional to the predischarge voltage in the higher level ranges. ESD Waveforms. Electrostatic discharge is typically broken down into two primary types of discharge: human (direct) and furniture (air), illustrated in Figure 7.7. Human discharge is characterized by a fast rise of current, approximately 1 ns, up to a peak of 10 A, followed by a decay back to zero. With this waveform, significant RF energy is present up to 300 MHz. Furniture discharge has a slower rise of current to a peak of 40 A, followed by damped oscillations. For this waveform RF energy is observed up to 30 MHz.
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Figure 2.2. Classes and examples of common metallo-organic starting compounds used in chemical solution deposition processing. A common feature for all compounds is M O C bonding. Associated structures are also shown. [Adapted with permission from Ref. 8: R. W. Schwartz et al., C. R. Chemie, 7, 433 (2004).]
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based on the SSN. When operating as a relay point, the SG behaves like a STP within the IP network: it may route the connection to an intermediate IP node based on SCCP and MTP3 address information and may perform GTT when receiving a GT address. Intermediate SUA nodes can also behave as relay points, resulting in multihop SCTP connections. The relay mode is optional and can be used for network scaling purposes. For connectionless communication, each SCCP message is routed individually. For connection-oriented communication, after routing the Connection Request, the SG maps the SCCP connection on the SCN side to the SCTP association on the IP side. SCCP User messages are transported between SUA nodes in CO and CL class messages such as Connectionless Data Transfer (CLDT) and Connection-Oriented Data Transfer (CODT). The formats for those messages are rather complex, and for their formats and a complete list of messages the reader is referred to [24]. Functionality equivalent to SUA can also be provided by M3UA, but SUA is optimized for SSCP User applications and results in a leaner protocol stack in the ASP. With SUA, only the SG requires SCCP functionality and multiple application servers are reachable from a single SG, although they do not have point codes and appear to SS7 entities in the SCN as residing in one node.
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FIGURE 13.6 UDP multipath condition from results of ray-tracing simulation and a channel pro le with 200 MHz.
This is the classical Maxwell-Boltzmann limit of the Fermi-Dirac distribution function, where the Fermi level EF, has a clear thermodynamic interpretation. The Euler relation in thermodynamics relates the total internal energy in the semiconductor to the intensive variables, temperature (T), pressure (P), chemical
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SOURCE SIZE MEASUREMENT that the maximum permissible power divided by the square root of the spot area remains constant whether the tube is run at 30, 40 or 50 kV. This is in agreement with the results of M ller (M ller, u u 1931) and Oosterkamp (Oosterkamp, 1948). The maximum loading is a fortuitously close to an easily remembered value, namely 1 W m 1 .
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