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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Rheologica acta 28 (1989), S. 464-472 
    ISSN: 1435-1528
    Keywords: Slit die viscometer ; viscous heating correction ; Weissenberg-Rabinowitch operator ; time-temperature superposition principle
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: Abstract If the viscosity can be expressed in the formη = α (T)f(σ), the walls are at a constant temperatureT 0, and the extra stress, velocity and temperature fields are fully developed, then the wall shear rate $$\dot \gamma _w$$ can be calculated by applying the Weissenberg-Rabinowitsch operator toF c Q instead of to the flow rateQ, whereF c is a correction factor which differs from 1 when the temperature field is non-uniform; the isothermal equation relating the wall shear stress and pressure gradient is still valid. For the case in whcihη = η 0|σ| n /(1 +β(T−T 0)), wheren, η 0, andβ are independent of shear stressσ and temperatureT, an exact analytical expression forF c in terms of the Nahme-Griffith numberNa andn is obtained. Use of this expression gives agreement with data obtained for degassed decalin (η = 2.5 mPa s) from a new miniature slit-die viscometer at shear rates $$\dot \gamma$$ up to 5 × 106s−1; here, the correction is only 7%,Na is 1.3, andGz, the Graetz number at the die exit, is 119. For a Cannon standard liquidS6 (η = 9 mPa s), agreement extends up to 5 × 105s−1; at 2×106s−1 (whereNa = 7.2 andGz = 231), the corrections are 11% (measured) and 36% (calculated).
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Rheologica acta 30 (1991), S. 357-368 
    ISSN: 1435-1528
    Keywords: Slit die viscometer ; developing thermal field ; viscous heating correction ; finite element method
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology , Physics
    Notes: Abstract In the thermally developing region, dπ yy /dx| y=h varies along the flow direction x, where π yy denotes the component of stress normal to the y-plane; y = ±h at the die walls. A finite element method for two-dimensional Newtonian flow in a parallel slit was used to obtain an equation relating dπ yy /dx/ y=h and the wall shear stress σω0 at the inlet; isothermal slit walls were used for the calculation and the inlet liquid temperature T0 was assumed to be equal to the wall temperature. For a temperature-viscosity relation η/η0 = [1+β(T−T0]−1, a simple expression [(hdπ yy /dx/ y=h )/σ w0] = 1−[1-F c(Na)] [M(χ)+P(Pr) ·Q(Gz −1)] was found to hold over the practical range of parameters involved, where Na, Gz, and Pr denote the Nahme-Griffith number, Graetz number, and Prandtl number; χ is a dimensionless variable which depends on Na and Gz. An order-of-magnitude analysis for momentum and energy equations supports the validity of this expression. The function F c(Na) was obtained from an analytical solution for thermally developed flow; F c(Na) = 1 for isothermal flow. M(χ), P(Pr), and Q(Gz) were obtained by fitting numerical results with simple equations. The wall shear rate $$\dot \gamma _{w0} $$ at the inlet can be calculated from the flow rate Q using the isothermal equation.
    Type of Medium: Electronic Resource
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