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Electrical current increasing temperature

Semiconductors, Semiconductors have resistivities much smaller than those of insulators and much greater than those of most metallic conductors. The conduction of electricity in semiconductors is achieved by carriers which may be either occasional excess electrons loosely bonded to lattice positions or holes created by an absence of electrons at scattered lattice spaces. In the presence of an electric field the electrons can migrate through the lattice and conduct an electric current. The temperature coefficient of resistance of semiconductors is negative (i.e., the resistance decreasing with increasing temperature) because the increased thermal vibrations accompanying an increase in temperature promote the transition of a carrier from one lattice point to the next. [Pg.85]

Tellurium is diamagnetic below its melting point. Its intrinsic electrical resistivity at room temperature is about 0.25 ohmcm, when the current is parallel to the i -axis, and decreases with increasing temperature and pressure. The element forms a continuous range of isomorphous solutions with selenium, consisting, in the soHd state, of chains of randomly alternating Se and Te atoms. [Pg.384]

The ions move between electrodes in the electrolyte due to voltage potential gradients. The velocity of these chemical currents increases with temperature. Hence, electrolytic conductivity increases as temperature goes up. This is the opposite of electrical currents m metallic conductors, which increase as the temperature goes down. [Pg.116]

Seebeck s outstanding scientific achievement was the discovei"y of one of the three classical thermoelectric effects, which are the Seebeck, the Peltier, and the Thomson effects. Seebeck s discovery was the first, dating from 1822—1823, followed by that of Jean-Charles-Athanase Peltier in 1832 and that of William Thomson in 1854. Seebeck obseiwed that an electric current in a closed circuit comprised different metallic components if he heated the junctions of the components to different temperatures. He noted that the effect increases linearly with the applied temperature difference and that it crucially depends on the choice of materials. Seebeck tested most of the available metallic materials for thermoelectricity. His studies were further systematized by the French physicist... [Pg.1038]

Metals and semiconductors are electronic conductors in which an electric current is carried by delocalized electrons. A metallic conductor is an electronic conductor in which the electrical conductivity decreases as the temperature is raised. A semiconductor is an electronic conductor in which the electrical conductivity increases as the temperature is raised. In most cases, a metallic conductor has a much higher electrical conductivity than a semiconductor, but it is the temperature dependence of the conductivity that distinguishes the two types of conductors. An insulator does not conduct electricity. A superconductor is a solid that has zero resistance to an electric current. Some metals become superconductors at very low temperatures, at about 20 K or less, and some compounds also show superconductivity (see Box 5.2). High-temperature superconductors have enormous technological potential because they offer the prospect of more efficient power transmission and the generation of high magnetic fields for use in transport systems (Fig. 3.42). [Pg.249]

Ionic (electrolytic) conduction of electric current is exhibited by electrolyte solutions, melts, solid electrolytes, colloidal systems and ionized gases. Their conductivity is small compared to that of metal conductors and increases with increasing temperature, as the resistance of a viscous medium acts against ion movement and decreases with increasing temperature. [Pg.100]

Later, the conductivity also did not change in spite of the presence of CP ions, which ought to be less solvated due to much smaller size compared to sulphate ions, were still not available for conducting electrical current as these were systematically removed from the solution and were taken inside the co-ordination shell of the Cu (II) complex. Therefore, the total number of active chloride ions was much less and hence the electrical conductivity did not rise in spite of an increase in the temperature of the solution by about 10°C (Table 9.5a). The increase in the electrical conductance in the last experiment, with CuCl2 (Table 9.5c), however, showed an increased chloride ion activity with rise in temperature, in spite... [Pg.234]

In ultra pure crystalline silicon, there are no extra electrons in the lattice that can conduct an electric current. If however, the silicon becomes contaminated with arsenic atoms, then there will be one additional electron added to the silicon crystal lattice for each arsenic atom that is introduced. Upon heating, some of those "extra electrons will be promoted into the conduction band of the solid. The electrons that end up in the conduction band are able to move freely through the structure. In other words, the arsenic atoms increase the conductivity of the solid by providing additional electrons that can carry a current when they are promoted into the conduction band by thermal excitation. Thus, by virtue of having extra electrons in the lattice, silicon contaminated with arsenic will exhibit greater electrical conductance than pure silicon at elevated temperatures. [Pg.255]

Positive temperature coefficient (PCT) thermistors are solids, usually consisting of barium titanate, BaTiOi, in which the electrical resistivity increases dramatically with temperature over a narrow range of temperatures (Fig. 3.38). These devices are used for protection against power, current, and thermal overloads. When turned on, the thermistor has a low resitivity that allows a high current to flow. This in turn heats the thermistor, and if the temperature rise is sufficiently high, the device switches abruptly to the high resisitvity state, which effectively switches off the current flow. [Pg.126]

Warming iron or steel to a temperature of about 500 °C causes it to glow a dull red colour, as seen on an electric cooker set at Tow . The oven ring appears bright orange if the temperature increases further ( 1000°C). In these kitchen items, an electric current inductively heats a coil of wire. [Pg.473]

Figure 2.1 A bomb calorimeter. The food is ignited by an electric current within the inner compartment, which is known as the bomb because the reaction within the box is generally so rapid as to be almost explosive. Insulation prevents heat loss and the thermometer measures the rise in temperature of the water that surrounds the bomb. From this increase, and the thermal capacity of the apparatus, the amount of heat released can be calculated. Figure 2.1 A bomb calorimeter. The food is ignited by an electric current within the inner compartment, which is known as the bomb because the reaction within the box is generally so rapid as to be almost explosive. Insulation prevents heat loss and the thermometer measures the rise in temperature of the water that surrounds the bomb. From this increase, and the thermal capacity of the apparatus, the amount of heat released can be calculated.
When an electric current is passed through a conductive medium, heat is generated (Joule heating). The temperature increase depends on the power,... [Pg.26]

Note that as the coolant flow rate is increased at lower rates, the capability of the heat sink to remove thermal energy is enhanced. This effect has diminishing retnrns at high rates due to the increased dependency on condnctive rather than convective heat transfer. At low flow rates and at reduced effective heat-transfer coefficients, the resnlts are somewhat impractical. In these cases, adjacent IGBTs are not maintained at equal temperatures. This condition would generate imbalances in the electrical current sharing, resulting in nndesirable switch performance. [Pg.100]


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See also in sourсe #XX -- [ Pg.437 ]




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