IMPELLER DRAFT TUBE AGITATION SYSTEM FOR GAS-LIQUID MIXING IN A STIRRED TANK REACTOR
The present invention relates to an improved design for the agitation system in stirred tank reactors for gas-liquid reactions. In particular the present invention relates to a system which incorporates a draft tube, one or more axial impellers and one or more radial impellers. The new agitation design offers improved contact between a liquid phase and a gaseous phase within the reactor.
Stirred Tank Reactors (STRs), in which gas and liquid phases make intimate contact for mass transfer, are very common in chemical processes such as fermentation, hydrogenation, phosgenation, neutralization, chlorination, and organic oxidation. The design of the STR has a significant effect on gas bubble dispersion, interfacial area ("a"), bubble surface transience, and the mass transfer coefficient "KL". These factors in turn effect the rate of conversion, selectivity and the yield of the reaction. The design of the STR also has an impact on the power needed to run the impeller system at a given rate.
Many different mixing systems have been reported in the art to try and achieve the maximum mass transfer between the gas and liquid phases. These include U.S. Patents 4,231,974; 5108,662; 5,371,283; 5,451,349; 5,523,474; 5,536,875; 5,696,285. These prior mixing attempts can be improved, as they do non have optimal mass transfer coefficients nor have they minimized the power requirements.
The present invention incorporates a draft tube along with both axial impeller and radial impellers. The axial impeller(s) is (are) located inside the cylinder formed by the draft tube, while the radial impeller(s) is located below the cylinder formed by the draft tube. The fluid flow and the mass transfer characteristics of such a system are superior to the conventional agitation system.
Additional advantages and features of the present invention will become apparent from a reading of the detailed description of the invention which makes reference to the following drawing.
Figure 1 is a cross-sectional view of an apparatus which corresponds to the present invention.
Figure 2 is a graph of observed Kj_a vs. gas flow rate for three different agitation rates in a system having a draft tube.
Figure 3 is a graph of observed Kj^a vs. gas flow rate for three different agitation rates in a system not having a draft tube.
As seen in Figure 1 , the present invention comprises a shaft 1 ; at least one axial impeller 2 attached to the shaft 1 , for moving fluid in a direction generally parallel to the shaft's axis 1 1 ; at least one radial impeller 3 attached to the shaft 1, for moving fluid in a direction generally perpendicular to the shaft's axis 1 1 ; and a draft tube 4 in the shape of a generally open cylinder. As is clearly shown in Figure 1 , when the agitation system 5 is placed within a stirred tank reactor 10, the shaft 1 extends through the draft tube 4 and the one or more axial impellers 2 are located within the draft tube cylinder 4 and the one or more radial impellers 3 are located outside of the draft tube cylinder 4.
The stirred tank reactor 10 with the agitation system 5, should be arranged in a vertical fashion as presented in Figure 1 , such that the radial impellers 3 are located below the draft tube 4. Also as shown in Figure 1, the entrance to the draft tube 4 is preferably beveled away from the shaft 1 , although this is not mandatory.
As the shaft 1 rotates around its axis 1 1 , the axial impellers 2 act to move the reactor contents down through the draft tube 4 in a direction generally parallel to the shaft's axis 1 1. Axial impellers are generally known in the art and any such impellers may be used in the present invention. For example, a double helix impeller such as the one depicted in U.S. 5,108,662, or an airfoil blade impeller such as the one depicted in U.S. Patent 4,231,974 could be used in this invention. Other suitable axial impellers include Pitch Blade Turbine, high efficiency impellers (such as model A-310 from Lightnin Mixing Co, HE-3 from Chemineer, Inc. and Viscoprop from EKATO Rueher and Mischtechnik GmbH), single helixes or marine props (such as A-315 or A-320 from Lightnin Mixing Co., MT-4, or MY- 4 from Chemineer, Inc.). The number of axial impellers used in general depends on the viscosity of the working media. The more viscous the working media the more axial impellers are warranted. It is contemplated that the invention may comprise from 1 to several axial impellers 2, but it is preferred that there be two.
Simultaneously, as the shaft 1 rotates around its axis 11 , the radial impellers 3 act to move the reactor contents away ,rom the shaft 1, and (as the radial impellers 3 are located below the draft tube 4) outside the draft tube 4. The center line of the radial impeller(s) should be far enough below the end of the draft tube to avoid substantial interference. This is typically in a range of from about 1/8 the distance of the radial impeller's diameter to about 7/8 of the radial impeller's diameter, with about 2/3 being most preferred. Radial impellers are also generally known in the art, and any design may be used in the current invention. Common radial impellers which are suited for use in the present invention include flat blade impellers, Rushton Impellers, Concave Disk Turbine (Smith turbine) SCABA (SRGT) impellers and model BT-6 from Chemineer, Inc. The optimum number of radial impellers to be used is dependent upon the ratio of the liquid height to the tank diameter. In most cases a single radial impeller will be used in the current invention, but in some reactors, such as tall fermenters, multiple radial impellers may be used.
Draft tubes and their modifications are also well known in the art, and those teachings are generally applicable to this invention. For example, the draft tube can be slotted to provide for return of liquid to the center of the draft tube if the level of liquid for some reason does not exceed the top of the draft tube. Also, the use of vertical baffles on the inner surface of the draft tube can be advantageously used to redirect tangential flow to axial flow. If baffles are used in the draft tube it is preferred that they have a width of 0.8 to 0.1 of the draft tube inner diameter with a clearance of 0.016 to 0.021 of the draft tube inner diameter. Moreover, the use of a baffle to partially close of the bottom of the cylinder formed by the draft tube is shown, inter alia, in U.S. Patent 5,536,875 and may also be used in the present invention.
Although the dimensions of the draft tube 4 are not critical to the present invention, it has been found that the optimum radius of the draft tube is 0.707 of the tank radius. Using a draft tube of this radius make the cross sectional area of the tank which is inside the draft tube equal the cross sectional area of the tank which is outside the draft tube. As seen in Figure 1 , the draft tube 4 can optionally contain a conically flared portion 6, at the entrance end of the draft tube. It is believed that this section will aid in straightening the flow of the reactor contents. The angle of the bevel should be between 30 and 60 degrees, with 45 degrees being most preferred. The beveled edge should not be too long, such that it restricts
flow around the top of the draft tube. It is preferred if the length of the beveled edge is from zero to about one fourth of the draft tube's inner diameter, with about 1/12 of the length being most preferred.
The present invention can be used with stirred tank reactors of any dimensions. The draft tube can be held in the appropriate position using side structural braces which attach to the reactor wall, as is known in the art. Also along the reactor wall, baffles can be optionally used, as is generally known in the art. If used, there are preferably four baffles spaced approximately 90 apart from each other. The reactant gas can be brought into the tank by any apparatus known in the art. These include ring spargers and more preferably pipe or nozzle spargers.
It should be understood that specific details of construction of the invention, such as materials, dimensions and the like, are not to be considered as limitations of the invention. Rather, these details can be adjusted as needed to create a preferred embodiment of the invention for any particular application.
The effectiveness of the present invention may be seen in the following Examples:
EXAMPLES
A transient technique was used to determine the mass transfer coefficient. This dynamic gassing out technique consists of sparging the reactor with pure nitrogen until all oxygen has been stripped from the working media. The sparge gas is then rapidly changed from nitrogen to oxygen. The transient oxygen concentration is then measured. These measurements can then be used to calculate the volumetric mass transfer coefficient (K.La) for the system. Physical techniques such as this are applicable to a well mixed system and to small values of Kj^a due to the slow response time of dissolved oxygen probes. In general these physical techniques are applicable where Kj^a < 1/τ, where τ is the dissolved oxygen probe response time.
An ASME dish bottom PLEXIGLAS™ tank having a 0.45 m inner diameter (0.08m3) was used to conduct the gas-liquid mixing experiments. Four flat baffles spaced 90 apart, were used to facilitate axial mixing. The agitation system included two high-
efficiency down-pumping axial impellers (model A-310 from Lightnin Mixers Ltd.), and one radial gas dispersing Rushton disk turbine (Lightnin R-100). The gas was sparged through a ring sparger located below the radial impeller. Deionized water was used as the working media. The agitator speed and torque were measured by a proximity tachometer and load cell, respectively, while the concentration of dissolved oxygen in the water was measured with two oxygen sensors (Electrosense DO probes having a response time of 2 seconds for 95% saturation). The agitation levels (gassed power of 0.26 -2.6 watt/kg) were sufficient to create uniform gas dispersion at a 0.012 - 0.046 m/s (i.e. 1-5 VVM) superficial gas velocity. All of the data was collected using a CAMILE™ 2000 data acquisition system. The K.La at different gas flow rates and shaft speeds (power) was first determined for the system without a draft tube. ANSI/ASCE Standard 2-91 entitled "Measurement of Oxygen Transfer in Clean Water" was used with non-linear regression (such as in the statistical software package known as JMP from SAS Institute, Cary, North Carolina, U.S.A.) to determine the correlation between the Mass transfer coefficient, Kj^a (1/sec) and superficial gas velocity, Vsg (m/sec). These results are shown in Table 1 and graphically depicted in Figure 2.
Table 1
Mass Transfer Coefficient without the Draft Tube
Speed Gas flow rate Power per mass Superficial gas velocity Mass transfer coefficient N [rpm] Q [scfm] ε [w/kg] Vsg [m/s] kLa [1/sec]
300 4 2.66 0.0122 0.063
300 6 2.30 0.0182 0.070
300 9 2.14 0.0274 0.077
300 12 2.21 0.0365 0.081
250 4 1.66 0.0122 0.057
250 6 1.55 0.0182 0.058
250 9 1.49 0.0274 0.068
250 12 1.52 0.0365 0.072
250 15 1.49 0.0456 0.074
200 4 1.06 0.0122 0.043
200 6 1.02 0.0182 0.046
200 9 0.95 0.0274 0.053
200 12 0.96 0.0365 0.064
200 15 0.94 0.0456 0.067
Then a draft tube having an inner diameter of 0.3 m (to achieve approximately equal
superficial gas velocities in the draft tube and the annular region surrounding the draft tube) was placed in the mixing system. The was again determined at different gas flow rates and shaft speeds (power). The results with the draft tube are shown in Table 2 and depicted graphically in Figure 3.
Table 2 Mass Transfer Coefficient with the Draft Tube
Speed Gas Flow Rate Power per mass Superficial gas velocity Mass transfer coefficient N [φ ] Q [scfm] ε [w/kg] Vsg [m/s] kLa [1/sec]
300 4 2.21 0.0121 0.075
300 6 1.85 0.0182 0.081
300 9 1.53 0.0273 0.094
300 12 1.50 0.0365 0.099
300 15 1.45 0.0456 0.099
250 4 1.28 0.0121 0.062
250 6 1.08 0.0182 0.069
250 9 0.90 0.0273 0.075
250 12 0.85 0.0365 0.083
250 15 0.88 0.0456 0.092
200 4 0.70 0.0121 0.045
200 6 0.65 0.0182 0.051
200 9 0.61 0.0274 0.059
200 12 0.60 0.0365 0.063
200 15 0.52 0.0456 0.069
As seen from these results, the presence of the draft tube increases the Kj^a over that of a conventional system having no draft tube, increases the gas hold-up and decreases the power draw for the same motor speed.