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Volume 6, Issue 3
Reverse Roll Coating Flow with Non-Newtonian Fluids

Jiin-Yuh Jang & Peng-Yuan Chen

Commun. Comput. Phys., 6 (2009), pp. 536-552.

Published online: 2009-06

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  • Abstract

In this study an incompressible flow with non-Newtonian fluids in the reverse roll coating process was investigated. Non-Newtonian behavior of the coating fluid was accounted by using power law model with power index, n, ranging from 0.8 to 1.2. Effect of roll speed ratio (V2/V1) of the panel roll to the applicator roll and gap distance on the coating film thickness were also investigated. Numerical results were in good agreement with those of experimental data within 15%-20%. Results indicated that the film thickness ratios are function of power-law index, roll speed ration and ratio of roll radius to gap distance. The equations for film thickness ratio were obtained from numerical results as shown below:
where t1, t2 and t3 are inlet film, transferred film and leakage film thickness, respectively, n is power-law index, V1 and V2 are roll speed of applicator roll and panel roll, Rm is average radius of two rolls and H0 is gap distance. The correlations are accurate within 10% for 0.8≤n≤1.2, 0.5≤V2/V1≤2, and 7.7×10−5≤ H0/Rm ≤1.54×10−4.

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@Article{CiCP-6-536, author = {}, title = {Reverse Roll Coating Flow with Non-Newtonian Fluids}, journal = {Communications in Computational Physics}, year = {2009}, volume = {6}, number = {3}, pages = {536--552}, abstract = {

In this study an incompressible flow with non-Newtonian fluids in the reverse roll coating process was investigated. Non-Newtonian behavior of the coating fluid was accounted by using power law model with power index, n, ranging from 0.8 to 1.2. Effect of roll speed ratio (V2/V1) of the panel roll to the applicator roll and gap distance on the coating film thickness were also investigated. Numerical results were in good agreement with those of experimental data within 15%-20%. Results indicated that the film thickness ratios are function of power-law index, roll speed ration and ratio of roll radius to gap distance. The equations for film thickness ratio were obtained from numerical results as shown below:
where t1, t2 and t3 are inlet film, transferred film and leakage film thickness, respectively, n is power-law index, V1 and V2 are roll speed of applicator roll and panel roll, Rm is average radius of two rolls and H0 is gap distance. The correlations are accurate within 10% for 0.8≤n≤1.2, 0.5≤V2/V1≤2, and 7.7×10−5≤ H0/Rm ≤1.54×10−4.

}, issn = {1991-7120}, doi = {https://doi.org/}, url = {http://global-sci.org/intro/article_detail/cicp/7691.html} }
TY - JOUR T1 - Reverse Roll Coating Flow with Non-Newtonian Fluids JO - Communications in Computational Physics VL - 3 SP - 536 EP - 552 PY - 2009 DA - 2009/06 SN - 6 DO - http://doi.org/ UR - https://global-sci.org/intro/article_detail/cicp/7691.html KW - AB -

In this study an incompressible flow with non-Newtonian fluids in the reverse roll coating process was investigated. Non-Newtonian behavior of the coating fluid was accounted by using power law model with power index, n, ranging from 0.8 to 1.2. Effect of roll speed ratio (V2/V1) of the panel roll to the applicator roll and gap distance on the coating film thickness were also investigated. Numerical results were in good agreement with those of experimental data within 15%-20%. Results indicated that the film thickness ratios are function of power-law index, roll speed ration and ratio of roll radius to gap distance. The equations for film thickness ratio were obtained from numerical results as shown below:
where t1, t2 and t3 are inlet film, transferred film and leakage film thickness, respectively, n is power-law index, V1 and V2 are roll speed of applicator roll and panel roll, Rm is average radius of two rolls and H0 is gap distance. The correlations are accurate within 10% for 0.8≤n≤1.2, 0.5≤V2/V1≤2, and 7.7×10−5≤ H0/Rm ≤1.54×10−4.

Jiin-Yuh Jang & Peng-Yuan Chen. (2020). Reverse Roll Coating Flow with Non-Newtonian Fluids. Communications in Computational Physics. 6 (3). 536-552. doi:
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