BATCH CONCENTRATION
Figure 1. Equation assumes liquid continues to contact the straight sides of the vessel.
DERIVING THE EQUATIONFor simplification, let’s assume the liquid is in a jacketed tank and remains on the straight side of the vessel as it is concentrated (Figure 1). For purposes of integration, let’s also assume the heat of vaporization (
ΔH), liquid density (
ρ), overall heat transfer coefficient (
U) and the temperature differential between the steam or other heat-transfer medium in the jacket and the liquid in the tank (
ΔT) remain constant. First, let’s consider the geometry of the batch as it remains on the tank straight side:The wetted area is:
AS = πDh (1) The volume relationship is:
VS = πD2h/4 (2)Dividing Eq. 1 by Eq. 2 provides the area-to-volume relationship:
AS/VS = 4/D (3)So, the total wetted area is:
AT = AH + 4(VT-VH)/D (4)Differentiating Eq. 4 with respect to time gives:
dAT/dt = (4/D)dVT/dt (5)Next, let’s write an alternative expression for
dVT/dt using the heat transfer rate and fluid properties:
dVT/dt = -Q/(ρΔH) (6)Substituting the standard expression for heat transfer yields:
dVT/dt = -UATΔT/ρΔH (7)Using Eq. 5 to eliminate volume in the relationship leads to:
(D/4)dAT/dt = -UATΔT/ρΔH (8)Solving for dA
T/dt gives:
dAT/dt = -4UATΔT/ρDΔH (9)At this point, it is convenient to define a characteristic time constant:
Θ = ρDΔH/4UΔT (10)Substituting Eq. 10 into Eq. 9 gives:
dAT/dt = -AT/Θ (11)Rearrangement yields:
dAT/AT = -dt/Θ (12)We then can solve Eq.12 per standard procedure:dln(A
T ) = -1/Θdt (13)Integrating to the indefinite solution gives:
ln(AT) = -t/Θ (14)Then, substituting the integration limits (A
t at time t, A
0 at time 0), we obtain:
ln(At/A0) = <-t/Θ (15)Rewriting Eq. 15 provides the following simple equation:
At/A0 = e–t/Θ (16)where Θ is given by Eq. 10.
PROCESS EXAMPLEWe want to concentrate a batch from 735 gal to 617 gal in a 5-ft-diameter tank. The bottom head holds 74 gal and provides 23 ft
2 of wetted area, in addition to the jacket. The solvent has a heat of vaporization of 1,036 Btu/lb and a density of 62.3 lb/ft
3. We can assume the overall heat transfer coefficient is 50 Btu/(hr∙ft
2∙°F). What is the time to evaporate the batch if the ΔT across the jacket is maintained at 165°F?First, we must convert volumes to cubic feet:
V0 = 735/7.481 = 98.25 ft3Vt = 617/7.481 = 82.48 ft3VH = 74/7.481 = 9.89 ft3Then, we calculate wetted areas per Eq. 4:
A0 = 23 + 4(98.25 - 9.89)/5 = 93.7 ft2
At = 23 + 4(82.48 - 9.89)/5 = 81.1 ft2
From Eq. 10, we determine characteristic time:
Θ = (62.3 × 5 × 1,036)/(4 × 50 × 165) = 9.78 hr
Using a rearrangement of Eq. 15 we get:
t = -Θ ln(At/A0) = - 9.78 ln(81.1/93.7) = -9.78 ln(0.8655) = 1.4 hr
So, the time needed to concentrate the batch from 735 gallons to 617 gallons is 1.4 hr.
MICHAEL J. GENTILCORE is Hazelwood, Mo.-based chemical process engineering manager for Mallinckrodt, a business unit of Covidien that will become a standalone company in 2013. E-mail him at [email protected]
NOMENCLATURE
A Area, ft2
D Tank diameter, ft
h Liquid height above head, ft
ΔH Heat of vaporization, Btu/lb
Q Heat transfer rate, Btu/hr
ΔT Temperature difference between jacket and process, °F
t Time, hr
U Overall heat transfer coefficient, Btu/(hr∙ft2∙°F)
V Volume, ft3
ρ Liquid density, lb/ft3
Θ Time constant (per Eq. 10), hr
Subscripts
0 Time zero
H Bottom head
S Straight side of vessel
T Total
t Time t
REFERENCES
1. Kern, D. Q., “Process Heat Transfer,” p. 624, McGraw-Hill, New York (1950) [still available in McGraw-Hill Classic Textbook Reissue Series].
2. Green, D. W. and Perry, R. H., “Perry’s Chemical Engineers’ Handbook,” 6th Ed., p. 10-38, McGraw Hill, New York (1997).
3. Gentilcore, M. J., “Estimate Heating and Cooling Times for Batch Reactors,” p. 41, Chem. Eng. Progress (March 2000).