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Energy, units thermal expansion, coefficient

The thermal pressure coefficients of the pure polymers can be estimated from the ratio of thermal expansion coefficient, a, to isothermal compressibility, Px, as y = a/px. In the case where y is not available from the literature it can be calculated from solubility parameters which themselves are related to the cohesive energy density (C.E.D.) and hence to the strength of the internal pressure of the structural molecules u5). The binary parameter, S2/S, is obtainable from the method of group contribution given by Bondi116. It can alternatively be calculated by casting shadows of models of the molecules for various orientations, where the area for the monomer unit is estimated from the area of the projections. [Pg.161]

This version of the thermal energy can be considered appropriate especially for liquids characterized by large values of the thermal expansion coefficient and subject to large pressure gradients this can be the case for microchannels in which large pressure drops per unit length are ordinary for low hydrauhe diameters. [Pg.3445]

Here Q(t) denotes the heat input per unit volume accumulated up to time t, Cp is the specific heat per unit mass at constant pressure, Cv the specific heat per unit mass at constant volume, c is the sound velocity, oCp the coefficient of isobaric thermal expansion, and pg the equilibrium density. (4) The heat input Q(t) is the laser energy released by the absorbing molecule per unit volume. If the excitation is in the visible spectral range, the evolution of Q(t) follows the rhythm of the different chemically driven relaxation processes through which energy is... [Pg.272]

Probe Thermometers. Volume expansion thermometers use the expansion of liquids with rising temperature through a narrow tube. The expansion coefficient, defined as the increase in volume per unit volume per unit rise in temperature, is 0.00018 per Kelvin for mercury and 0.00109 per Kelvin for ethyl alcohol colored with dye. Calculating temperature from the actual random thermal motion velocity of every molecule, or the energy contained in a vibrational excitation of every molecule, is impractical. So temperature is measured indirectly in most applications. Different metals expand to different extents when their temperature rises. This difference is used to measure the bending of two strips of metal attached to one another in outdoor thermometers. Thermocouples use the Seebeck or thermoelectric effect discovered by Cerman physicist Thomas Johann Seebeck, in which a voltage difference is produced between two junctions between wires of... [Pg.1825]

The summation convention over repeated indices is assumed. Here an asterisk denotes some constant reference value taken, say, at the undisturbed interface. Besides, q denotes density and p, pressure. Vi and T denote the i-th component of the velocity field and temperature, respectively, T] is the shear or dynamic viscosity, rj = gu with u the kinematic viscosity, Cp the specific heat at constant pressure, g is the acceleration due to gravity and e the unit normal vector along z. a is the coefficient of thermal expansion. In eq. (3) we have also used the simplest caloric equation, of state between energy and temperature. To a first approximation the heat (J ) flux is... [Pg.90]


See other pages where Energy, units thermal expansion, coefficient is mentioned: [Pg.75]    [Pg.458]    [Pg.681]    [Pg.281]    [Pg.4831]    [Pg.192]    [Pg.14]    [Pg.95]    [Pg.281]    [Pg.630]    [Pg.837]    [Pg.78]    [Pg.459]    [Pg.198]    [Pg.84]    [Pg.630]    [Pg.122]    [Pg.174]    [Pg.551]    [Pg.708]   


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