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Cable coaxial

Waveguides are coimnonly used to transmit microwaves from the source to the resonator and subsequently to the receiver. For not-too-high-frequency radiation (<10 GHz) low-loss MW transmission can also be achieved usmg strip-lines and coaxial cables. At the output of a klystron an isolator is often used to prevent back-reflected microwaves to perturb the on-resonant klystron mode. An isolator is a microwave-ferrite device that pemiits the transmission of microwaves in one direction and strongly attenuates their propagation in the other direction. The prmciple of this device involves the Faraday effect, that is, the rotation of the polarization... [Pg.1559]

Electrical Applications. The largest application of PTFE is for hookup and hookup-type wire used in electronic equipment in the military and aerospace industries. Coaxial cables, the second largest appHcation, use tapes made from fine powder resins and some from granular resin. Interconnecting wire appHcations include airframes. Other electrical appHcations include computer wire, electrical tape, electrical components, and spaghetti tubing. [Pg.355]

Data Communication Wires. Electronic cables such as data communication wires employ three basic designs coaxial, twisted pair, and fiber optics (3,4) (Eig. 1). Coaxial cables are so named because the axis of curvature of its outer conductor is concentric to its inner central wire. The metal braiding wrapped around the insulated center wire acts as the return current conductor in addition to shielding the wire from various interferences. [Pg.322]

Eig. 1. Cable designs (a) coaxial cable (b) twisted pair cable can be unshielded, as in regular telephone wiring, or shielded (as shown here) with braiding or... [Pg.322]

For coaxial cables, the following electrical properties related to the dielectric constant of the core material and the dimensions determine the quaUty of the signal impedance, capacitance, attenuation, crosstalk, and time delay and velocity of propagation. [Pg.326]

Impedance. Impedance defines the relationship of voltage and current in a coaxial cable. The electrical requirements of the hardware dictate the impedance values for the interconnecting cables. Most coaxial cables are designed to match the impedances required by electronic hardware. [Pg.326]

Another type of electronic connector joins coaxial conductors. These have a soHd or stranded center-conductor surrounded by a dielectric. The dielectric is covered with a conductive shield made of metal braid or tape and with a layer of insulation. Coaxial cable connectors terminate the center-conductor and the shield. These are used primarily in radio frequency circuits. The shape, dimensions, and materials of an electronic connector shell or stmcture may have to be designed to shield the connection from electromagnetic and radio frequency interferences in many appHcations. [Pg.26]

Experimental studies within the elastic range have been performed on monocrystalline AI2O3 (sapphire) and the nonpiezoelectric z-cut of quartz. Experiments are performed with a circuit devised by Ingram [68G05] in which a low-loss coaxial cable is used for both application of the potential and monitoring the current. As shown in Fig. 4.7, at an applied potential difference of a few kilovolts, a current of about 1 mA is produced at a compression of several percent. [Pg.86]

In these and other applications where the coiled cable distorts or interferes with the accuracy of acquired data, a shielded coaxial cable should be used. While these non-coiled cables can be more difficult to use in conjunction with a portable analyzer, they are essential for low-speed and electromagnetic field applications. [Pg.690]

The other approach to the reduction of the power loss to the dielectric material is by reducing the amount used. This is done by replacing part of the dielectric by air, an inert gas, or by vacuum. As examples there are three cable constructions in common use which employ these approaches to minimize dielectric loss. The first is the use of a foamed dielectric PS plastic that is commonly used in either twin lead transmission lines or in coaxial cables used for antenna lead-in wires in the UHF-TV antenna applications. The second system, which is illustrative of several sectional spacers, is used widely in communications cables of the coaxial type to minimize losses to the dielectric by reducing the amount of dielectric material in the cable. [Pg.225]

Time domain reflectrometry Sends pulses through a cable and observes the reflected waveform, which is correlated to soil moisture Consists of a cable tester (or specifically designed commercial time domain reflectrometry unit), coaxial cable, and a stainless steel probe... [Pg.1081]

On the RF time scale, the transit times of electrons in long coaxial cables and the time of flight of photons in optical paths as short as a few centimeters are significant. These effects become more pronounced as the modulation frequency increases. Even simple changes made to a system will affect the resulting measurements. [Pg.89]

The radiation detector is located some distance from the readout. A shielded coaxial cable transmits the detector output to the amplifier. The output signal of the detector may be as low as 0.01 volts. A total gain of 1000 is needed to increase this signal to 10 volts, which is a usable output pulse voltage. There is always a pickup of noise in the long cable run this noise can amount to 0.001 volts. [Pg.82]

The matrix can be taken away by HN03 except at the ends of the wire, to allow easy soldering. Below IK, the electrical contact can be done also by squeezing the wires to be connected inside a thin A1 tube (see, for example, Section 12.4). For low-level signals, shielded twisted pairs or cryogenic coaxial cables are used. When thousands of wires are necessary, as in large experiments, Kapton strips with deposited conductors [3] or woven wires [4] are used. [Pg.105]

Capacitance measurements are quite simple. A typical drawback is the need of coaxial cables that introduce a thermal load which is not negligible in low-power refrigerators. On the other hand, capacitance bridges null the cable capacitance. Multiplexing is more difficult than for resistance thermometers. In principle, capacitors have low loss due to Joule heating. This is not always true losses can be important, especially at very low temperatures. Dielectric constant thermometers have a high sensitivity capacitance differences of the order of 10-19F can be measured. [Pg.227]

There are four types of buried sensors that rely on different types of triggers pressure or seismic magnetic field ported coaxial cable and fiber-optic cables. These four sensors are all covert and terrain-following, meaning they are hidden from view and follow the contour of the terrain. The four types of sensors are described in more detail below. Table 9.9 presents the distinctions between the four types of buried sensors. [Pg.177]

Ported coaxial cables Responds to motion of a material with a high dielectric constant or high conductivity near the cables... [Pg.179]

Buried-line ported coaxial cable sensors detect the motion of any object (i.e., human body, metal, etc.) possessing high conductivity and located within close proximity to the cables. An intruder entering into the protected space creates an active disturbance in the electric field, thereby triggering an alarm condition. [Pg.180]

Nanocarbon hybrids have recently been introduced as a new class of multifunctional composite materials [18]. In these hybrids, the nanocarbon is coated by a polymer or by the inorganic material in the form of a thin amorphous, polycrystalline or single-crystalline film. The close proximity and similar size domain/volume fraction of the two phases within a nanocarbon hybrid introduce the interface as a powerful new parameter. Interfacial processes such as charge and energy transfer create synergistic effects that improve the properties of the individual components and even create new properties [19]. We recently developed a simple dry wrapping method to fabricate a special class of nanocarbon hybrid, W03 /carbon nanotube (CNT) coaxial cable structure (Fig. 17.2), in which W03 layers act as an electrochromic component while aligned... [Pg.458]

Coaxial cable connectors, terminal and high voltage insulators transformers, relays, antennae, power amplifier components. .. [Pg.106]

Fig. 12. A flash photolysis apparatus. 1, high-voltage power supply 2, 10 M12 resistor 3. high-voltage capacitor 4, coaxial cable 5, flash tube 6, vacuum system 7, reflector 8, pulsed spectroscopic light source 9, measuring cell 10, Hilger medium quartz spectrograph. (From Vallotton and Wild, Ref. ))... Fig. 12. A flash photolysis apparatus. 1, high-voltage power supply 2, 10 M12 resistor 3. high-voltage capacitor 4, coaxial cable 5, flash tube 6, vacuum system 7, reflector 8, pulsed spectroscopic light source 9, measuring cell 10, Hilger medium quartz spectrograph. (From Vallotton and Wild, Ref. ))...
If a coaxial cable is used to connect the tunneling tip to the input of the amplifier, a major source of noise is the capacitance of the coaxial cable itself. The typical capacitance between the center conductor and the shielding is 100 pF per meter. In response to the acoustic noise in the room, the coaxial cable deforms. The capacitance changes. The current is... [Pg.256]

For example, if the voltage on the coaxial cable is 10 mV, a noise of 1 kHz makes a periodic change of capacitance with an amplitude of 1 pF, and the noise current is 60 pA, a tangible value. The phenomenon is the same as the principle of the capacitance microphone used in almost every portable tape recorder. To avoid such a microphone effect, the best way is to connect the current amplifier as close to the current source as possible and eliminate the coaxial cable. Almost every commercial STM uses such an arrangement. [Pg.256]

The coaxial cable is the major source of noise for yet another reason. At the input of the op-amp, there is always a small voltage noise, which is amplified by the op-amp and appears at the output end. To make a simplified analysis, let the input noise be represented by an ac source at the noninverting input end. The output voltage is (see Fig. 11.3)... [Pg.256]


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