Abstract:Gas flow characteristics in opaque fibre suspensions have been captured on film using a stop‐motion X‐ray imaging technique called flash X‐ray radiography (FXR). Gas flows in a bubble column filled with various cellulose fibre suspensions from 0% (an air–water system) to 5% by mass have been observed. The gas flow regime changes from vortical to churn‐turbulent as the fibre concentration increases for a fixed superficial gas velocity. Two new gas flow regimes, identified as surge churn‐turbulent and discrete c… Show more
“…When 0.6% ::; C ::; 1.5%, only the vortical-spiral flow and turbulent flow regimes appear, and the superficial gas velocity at which transition occurs is 13-14 cm/s, with the lower U. This is consistent with the observations of Reese et al [9] and Heindel [12] in semi-batch bubble columns. When Ug~5 cm/s, the slopes of the V g / e versus U g curves are not significantly different from those at C ::; 0.4%.…”
Section: Gas Flow Regime Transitionsupporting
confidence: 82%
“…Reese et al [9] found that in a 10.2 diameter cylindrical semi-batch bubble column filled with a fiber suspension, dispersed bubble, vortical-spiral, and turbulent flow could be identified when the fiber mass fraction was low (C S; 0.5%), while only dispersed bubble and turbulent flow were recordeã t high fiber mass fractions (C > 0.5%). In a I m t~1l2-D semibatch bubble column with a rectangular cross-secnon of 20 em x 2 em, Heindel [12] observed vortical, churn-turbulent, surge churn-turbulent and discrete channel flow as the fiber mass fraction increased from 0% to 5% with a fixed superficial gas velocity of 0.83 cm/s. In a 1.80 m tall 5.1 em diameter cocurrent bubble column, Xie et al [7] identified five distinct flow regimes in an air-water-cellulose fiber suspension, including dispersed bubbly, layered bubbly, (incipient plug and) plug, churn-turbulent, and slug flows.…”
Effects of superficial liquid velocity (Ul ), superficial gas velocity (Ug ), and fiber mass fraction (C) on gas holdup (ε) and flow regime transition are studied experimentally in well-mixed water-cellulose fiber suspensions in a cocurrent bubble column. Experimental results show that the gas holdup decreases with increasing Ul when C and Ug are constant. The gas holdup is not significantly affected by C in the range of C < 0.4%, but decreases with increasing C in the range of 0.4% ≤ C ≤ 1.5%. When C > 1.5%, a significant amount of gas is trapped in the fiber network and recirculates with the water-fiber slurry in the system; as a result, the measured gas holdup is higher than that at C = 1.5%. The axial gas holdup distribution is shown to be a complex function of superficial gas and liquid velocities and fiber mass fraction. The drift-flux model is used to analyze the flow regime transitions at different conditions. Three distinct flow regimes are observed when C ≤ 0.4%, but only two are identified when 0.6% ≤ C ≤ 1.5%. The superficial gas velocities at which flow transition occurs from one regime to another are not significantly affected by Ul and slightly decrease with increasing C.
ABSTRACTEffects of superficial liquid velocity (U/), superficial gas velocity (U g ), and fiber mass fraction (C) on gas holdup (c) and flowregime transition are studied experimentally in well-mixed water-cellulose fiber suspensions in a cocurrent bubble column. Experimental results show that the gas holdup decreases with increasingU/ when C and U g are constant. The gas holdup is notsignificantly affected by C in the range of C < 0.4%, but decreases with increasing C in the range of 0.4%~C ::; 1.5%.WhenC > 1.5%, a significant amount of gas is trapped in the fibernetwork and recirculates with the water-fiber slurry in the system; as a result, the measured gas holdup is higher than that atC::: 1.5%. The axial gas holdup distribution is shown to be a complexfunction of superficial gas and liquid velocities and fibermass fraction. The drift-flux model is used to analyze the flowregime transitions at different conditions. Three distinct flowregimes are observed when C~0.4%, but only two are identifiedwhen 0.6% s C s 1.5%. The superficial gas velocitiesat which flow transition occurs from one regime to another are not significantly affected by U/ and slightly decreasewith increasing C. KEYWORDS:Bubble column; Cellulose fiber; Gas holdup; Hydrodynamics;Multiphase flow
NOMENCLATUREBo coefficient in Eq. (3), Eo = COUI +U 1m C fiber mass fraction
“…When 0.6% ::; C ::; 1.5%, only the vortical-spiral flow and turbulent flow regimes appear, and the superficial gas velocity at which transition occurs is 13-14 cm/s, with the lower U. This is consistent with the observations of Reese et al [9] and Heindel [12] in semi-batch bubble columns. When Ug~5 cm/s, the slopes of the V g / e versus U g curves are not significantly different from those at C ::; 0.4%.…”
Section: Gas Flow Regime Transitionsupporting
confidence: 82%
“…Reese et al [9] found that in a 10.2 diameter cylindrical semi-batch bubble column filled with a fiber suspension, dispersed bubble, vortical-spiral, and turbulent flow could be identified when the fiber mass fraction was low (C S; 0.5%), while only dispersed bubble and turbulent flow were recordeã t high fiber mass fractions (C > 0.5%). In a I m t~1l2-D semibatch bubble column with a rectangular cross-secnon of 20 em x 2 em, Heindel [12] observed vortical, churn-turbulent, surge churn-turbulent and discrete channel flow as the fiber mass fraction increased from 0% to 5% with a fixed superficial gas velocity of 0.83 cm/s. In a 1.80 m tall 5.1 em diameter cocurrent bubble column, Xie et al [7] identified five distinct flow regimes in an air-water-cellulose fiber suspension, including dispersed bubbly, layered bubbly, (incipient plug and) plug, churn-turbulent, and slug flows.…”
Effects of superficial liquid velocity (Ul ), superficial gas velocity (Ug ), and fiber mass fraction (C) on gas holdup (ε) and flow regime transition are studied experimentally in well-mixed water-cellulose fiber suspensions in a cocurrent bubble column. Experimental results show that the gas holdup decreases with increasing Ul when C and Ug are constant. The gas holdup is not significantly affected by C in the range of C < 0.4%, but decreases with increasing C in the range of 0.4% ≤ C ≤ 1.5%. When C > 1.5%, a significant amount of gas is trapped in the fiber network and recirculates with the water-fiber slurry in the system; as a result, the measured gas holdup is higher than that at C = 1.5%. The axial gas holdup distribution is shown to be a complex function of superficial gas and liquid velocities and fiber mass fraction. The drift-flux model is used to analyze the flow regime transitions at different conditions. Three distinct flow regimes are observed when C ≤ 0.4%, but only two are identified when 0.6% ≤ C ≤ 1.5%. The superficial gas velocities at which flow transition occurs from one regime to another are not significantly affected by Ul and slightly decrease with increasing C.
ABSTRACTEffects of superficial liquid velocity (U/), superficial gas velocity (U g ), and fiber mass fraction (C) on gas holdup (c) and flowregime transition are studied experimentally in well-mixed water-cellulose fiber suspensions in a cocurrent bubble column. Experimental results show that the gas holdup decreases with increasingU/ when C and U g are constant. The gas holdup is notsignificantly affected by C in the range of C < 0.4%, but decreases with increasing C in the range of 0.4%~C ::; 1.5%.WhenC > 1.5%, a significant amount of gas is trapped in the fibernetwork and recirculates with the water-fiber slurry in the system; as a result, the measured gas holdup is higher than that atC::: 1.5%. The axial gas holdup distribution is shown to be a complexfunction of superficial gas and liquid velocities and fibermass fraction. The drift-flux model is used to analyze the flowregime transitions at different conditions. Three distinct flowregimes are observed when C~0.4%, but only two are identifiedwhen 0.6% s C s 1.5%. The superficial gas velocitiesat which flow transition occurs from one regime to another are not significantly affected by U/ and slightly decreasewith increasing C. KEYWORDS:Bubble column; Cellulose fiber; Gas holdup; Hydrodynamics;Multiphase flow
NOMENCLATUREBo coefficient in Eq. (3), Eo = COUI +U 1m C fiber mass fraction
“…When C > 0.6%, the slurry phase recirculation is suppressed, this was also reported by Lindsay et al (1995) and Heindel (2000Heindel ( ,2002, and is attributed to a decreased level of turbulence resulting from an increased slurry viscosity. This change in slurry flow characteristics results in fiber settling when Ug < 0.9 cm/s, causing a locally higher fiber mass fraction in the lower column region than in the upper column region.…”
Section: Effect Of Fiber Mass Fractionsupporting
confidence: 67%
“…However, fiber addition hindered small bubble coalescence in the cocurrent flow. In a semi-batch bubble column, Heindel (2000) observed that the number of small bubbles decreased and large bubbles increased with increasing fiber mass fraction. Bubbles rose upward in a serpentine flow pattern at low fiber mass fractions and this changed to a near vertical path at high fiber mass fractions.…”
Section: Bubble Behavior In Fiber Suspensionsmentioning
“…The presence of fibers can make the effective rheological properties of a fiber suspension significantly different from those of the suspending fluid [64][65][66]. Fiber floes or networks can significantly affect bubble motion, coalescence, and breakup, and thus, gas holdup in the bubble column [2,5,11,12,20,[67][68][69]. Pelton and Piette [69] reported that the main reason bubbles are held up in a fiber suspension is mechanical confinement, not bubble adhesion to fibers.…”
Gas-liquid-fiber systems are different from conventional gas-liquid-solid systems in that the solid material (i.e., fiber) is flexible, has a large aspect ratio, and forms flocs or networks when its mass fraction is above a critical value. With its wide application to the pulp and paper industry, it is important to investigate the hydrodynamics of gas-liquid-fiber systems. In this paper, 19 parameters that influence gas holdup in gasliquid-fiber bubble columns are critically examined and then a dimensional analysis based on the Buckingham Pi Theorem is used to derive the dimensionless parameters governing gas-liquid-fiber bubble column hydrodynamics. Seven dimensionless parameters that are related to the fiber effects on gas holdup are further analyzed, and a single dimensionless parameter combining these dimensionless parameters is derived based on a force analysis and experimental results. This dimensionless parameter is shown to be sufficient to quantify the influence of fiber on gas holdup in gas-liquid-fiber cocurrent bubble columns. It also reduces the number of parameters needed in correlating experimental gas holdup data in gas-liquid-fiber bubble columns.
ABSTRACTGas-liquid-fiber systems are different from conventional gas-liquid-solid systems in that the solid material (i.e., fiber) is flexible, has a large aspect ratio, and forms floes or networks when its mass fraction is above a critical value. With its wide application to the pulp and paper industry, it is important to investigate the hydrodynamics of gas-liquid-fiber systems.
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