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Temperature coefficient loss factor

An ultrasonic measuring system was developed to measure the attenuation coefficient/loss factor of car-tyre rubber samples as a function of the temperature between about -40°C and 150°C. These measurements were performed on sample disks of vulcanised rubber having a diameter of 60 mm. and a thickness of 13 mm. [Pg.111]

Tetralluoroethylene polymer has the lowest coefficient of friction of any solid. It has remarkable chemical resistance and a very low brittleness temperature ( — 100°C). Its dielectric constant and loss factor are low and stable across a broad temperature and frequency range. Its impact strength is high. [Pg.1016]

Sheet Miea. Good quahty sheet mica is widely used for many iadustrial appHcations, particularly ia the electrical and electronic iadustries, because of its high dielectric strength, uniform dielectric constant, low power loss (high power factor), high electrical resistivity, and low temperature coefficient (Table 6). Mica also resists temperatures of 600—900°C, and can be easily machined iato strong parts of different si2es and shapes (1). [Pg.291]

Activation Energy Using Loss Modulus or Loss Factor Curve -Activation energy can be determined either from peak loss modulus or peak loss factor temperature. Table IV compares the data obtained by either methods along with the correlation coefficient of the linear regression plots for determining activation energy. It is evident that either method is equally satisfactory, as would be expected. [Pg.143]

The equation will not always predict actual coating conditions. In this instance, tablet cores were coated in a partially perforated pan that limits the air volume passing through the tablet bed. A correction factor can be added to the model based on the partial perforation and metal mass of the pan. Ende and Berchielli have evaluated several coating pans and have included a heat loss factor in their calculations that relates the heat transfer coefficient and pan surface area. Their model is able to predict exhaust temperature in dissimilar coaters. [Pg.3212]

In a sequence of operations of the above kind the losses of the desired component A can be considerable, and the final amount of pure crystals may easily be a minute fraction of the starting mixture AB. This question of yield from recrystallization processes is of paramount importance, and many schemes have been designed with the object of increasing both yield and separation efficiency. The choice of solvent depends on the nature of the required substance A and the impurity B. Ideally, B should be very soluble in the solvent at the lowest temperature employed, and A should have a high temperature coefficient of solubility so that high yields of A can be obtained from operation within a small temperature range. Some of the factors affecting the choice of a solvent are discussed in section 3.2. [Pg.289]

As a matter of fact, the tolerance factor is a rather complex crystaUo-chemical parameter, which can reflect the structural distortion, force constants of binding, rotation and tilt of the BOg octahedrons. These in turn affect the dielectric properties, transition temperature, temperature coefficient of the dielectric constant of material, and even the dielectric loss behavior in a perovskite dielectric. [Pg.260]

Quantity of heat flowing through a 1 m area during one hour when there is a difference in the hot and cold side temperature of 1 K. It is also called the heat loss factor . (In the French and German technical literature, it is known as Coefficient k or k-wert , respectively). [Pg.466]

The required properties for dielectric resonator materials are (a) high dielectric constant (b) low dielectric loss tangent tan and (c) low temperature coefficient of resonant frequency Xj. Many kinds of dielectric resonator materials have been developed since the 1970s 128-311. Table 5.1.5 shows the dielectric properties of some materials that are commercially available now. In the table, the quality factor Q is reciprocal of dielectric loss tangent Q = If tan As tan S is proportional to frequency for ionic paraelectric materials, the product of Q and frequency is the value inherent to each material. Some materials have high Q value equal to copper cavity and some have the temperature coefficient as stable as Inver cavity. The material with lower 8j. generally has higher Q value. [Pg.175]

The fundamental parameters controlling operating characteristics of SAW-based sensors are the SAW velocity, the temperature coefficients of delay (TCD), the electromechanical coupling factor, and the propagation loss. In SAW applications, the coupling factor relates to the maximum bandwidth obtainable and the amount of signal loss between input and output that determines the fractional... [Pg.311]

Thermal breakdown is caused by the fact that d.c. conductivity results in Joule heating. Under an a.c. field, there is additional energy dissipation, with heat being generated in the dielectric materials faster than it can be dissipated to the surroundings. The subsequent rise in temperature will lead to an increase in conductivity and dielectric loss, which eventually culminates in a runaway situation and thermal breakdown. The breakdown voltage, Ub. is proportional to the thermal conductivity of the materials, X, the function

flat disc and the heat transfer coefficient), and is inversely proportional to the angular frequency of the a.c. field to, the temperature coefficient of the loss factor T, the dielectric permittivily e, and the loss factor tan 5 ... [Pg.312]

Radiation differs from conduction and convection not only in mathematical structure but in its much higher sensitivity to temperature. It is of dominating importance in furnaces because of their temperature, and in ciyogenic insulation because of the vacuum existing between particles. The temperature at which it accounts for roughly half of the total heat loss from a surface in air depends on such factors as surface emissivity and the convection coefficient. For pipes in free convection, this is room temperature for fine wires of low emissivity it is above red heat. Gases at combustion-chamber temperatures lose more than 90 percent of their energy by radiation from the carbon dioxide, water vapor, and particulate matter. [Pg.569]


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