Abstract
The results of a numerical study (using finite differences) of heat transfer in polymer melt flow is presented. The rheological behaviour of the melt is described by a temperature-dependent power-law model. The curved tube wall is assumed to be at constant temperature. Convective and viscous dissipation terms are included in the energy equation. Velocity, temperature and viscosity profiles, Nusselt numbers, bulk temperatures, etc. are presented for a variety of flow conditions.
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Abbreviations
- Br :
-
\(\eta _0 \bar \upsilon ^2 /\lambda t_0 \) — Brinkman number
- c :
-
specific heat, J/kg K
- De :
-
\(2r_p \bar \upsilon \varrho /(\eta _0 \exp ( - kt_0 )(r_p /r_c )^{1/2} )\) — Dean number
- E :
-
dimensionless apparent viscosity, eq. (14d)
- G :
-
dimensionless shear rate, eq. (19)
- k :
-
parameter of the power-law model, °C−1, eq. (7)
- \(\dot m\) :
-
mass flow rate, kg/s
- m 0 :
-
parameter of the power-law model, Pa · sn, eq. (7)
- n :
-
parameter of the power-law model, eq. (7)
- Nu :
-
2r pα/λ — Nusselt number, eqs. (28,31)
- p :
-
pressure, Pa
- Pe :
-
\(\bar \upsilon r_p \varrho c/\lambda \) — Péclet number
- P :
-
—(∂p/∂ϕ)/r c — pressure gradient, Pa/m
- \(\dot Q_d \) :
-
dissipated energy, W, eq. (29)
- \(\dot Q_t \) :
-
total energy, W, eq. (30)
- r :
-
radial coordinate, m
- r c :
-
radius of tube-curvature, m, fig. 1
- r p :
-
radius of tube, m, fig. 1
- r t :
-
variable, m, eq. (6)
- R :
-
dimensionless radial coordinate, eq. (14a)
- R c :
-
dimensionlessr c, eq. (14a)
- R t :
-
dimensionlessr t, eq. (14a)
- t :
-
temperature, °C
- \(\bar t\) :
-
bulk temperature, °C, eq. (27)
- t 0 :
-
inlet temperature of the melt, °C
- t w :
-
tube wall temperature, °C
- T :
-
dimensionless temperature, eq. (14c)
- T w :
-
dimensionless tube wall temperature
- T :
-
dimensionless bulk temperature
- u 1 :
-
variable, s−1, eq. (4)
- u 2 :
-
variable, s−1, eq. (5)
- U 1 :
-
dimensionlessu 1, eq. (18)
- U 2 :
-
dimensionlessu 2, eq. (18)
- v :
-
velocity inϕ-direction, m/s
- \(\bar \upsilon \) :
-
average velocity of the melt, m/s
- V :
-
dimensionlessv, eq. (14b)
- \(\bar V\) :
-
dimensionless\(\bar \upsilon \), eq. (15)
- z :
-
r cϕ — centre length of the tube, m
- Z :
-
dimensionlessz, eq. (14e)
- α :
-
heat transfer coefficient, W/m2 K
- \(\dot \gamma \) :
-
shear rate, s−1, eq. (8)
- \(\dot \gamma _0 \) :
-
\(\bar \upsilon /r_p \) — shear rate, s−1
- η :
-
apparent viscosity, Pa · s, eq. (7)
- η 0 :
-
\(m_0 \dot \gamma _0^{n - 1} \) — apparent viscosity, Pa · s
- θ :
-
angular coordinate, rad, fig. 1
- λ :
-
thermal conductivity, W/m K
- ϱ :
-
melt density, kg/m3
- ϕ :
-
axial coordinate, rad, fig. 1
- Δ :
-
rate of strain tensor, s−1, eq. (8)
- (—Δp):
-
pressure drop, Pa
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Závadský, E., Karniš, J. & Pechoč, V. Non-isothermal flow of polymer melts in a curved tube. Rheol Acta 24, 335–340 (1985). https://doi.org/10.1007/BF01333962
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DOI: https://doi.org/10.1007/BF01333962