Source code for fluids.mixing

"""Chemical Engineering Design Library (ChEDL). Utilities for process modeling.
Copyright (C) 2016, 2017, 2018, 2020 Caleb Bell <Caleb.Andrew.Bell@gmail.com>

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SOFTWARE.

This module contains some basic functions for fluid mechanics mixing
calculations.

For reporting bugs, adding feature requests, or submitting pull requests,
please use the `GitHub issue tracker <https://github.com/CalebBell/fluids/>`_
or contact the author at Caleb.Andrew.Bell@gmail.com.

.. contents:: :local:

Misc Functions
--------------
.. autofunction:: size_tee
.. autofunction:: COV_motionless_mixer
.. autofunction:: K_motionless_mixer
.. autofunction:: agitator_time_homogeneous
.. autofunction:: Kp_helical_ribbon_Rieger
.. autofunction:: time_helical_ribbon_Grenville

"""

from math import log, pi, sqrt

from fluids.constants import g

__all__ = ['agitator_time_homogeneous',
'Kp_helical_ribbon_Rieger', 'time_helical_ribbon_Grenville', 'size_tee',
'COV_motionless_mixer', 'K_motionless_mixer']

max_Fo_for_turbulent = 1/1225.
min_regime_constant_for_turbulent = 6370.

def adjust_homogeneity(fraction):
    '''Base: 95% homogeneity'''
    multiplier = log(1-fraction)/log(0.05)
    return multiplier


[docs]def agitator_time_homogeneous(N, P, T, H, mu, rho, D=None, homogeneity=.95): r'''Calculates time for a fluid mizing in a tank with an impeller to reach a specified level of homogeneity, according to [1]_. .. math:: N_p = \frac{Pg}{\rho N^3 D^5} .. math:: Re_{imp} = \frac{\rho D^2 N}{\mu} .. math:: \text{constant} = N_p^{1/3} Re_{imp} .. math:: Fo = 5.2/\text{constant} \text{for turbulent regime} .. math:: Fo = (183/\text{constant})^2 \text{for transition regime} Parameters ---------- N : float: Speed of impeller, [revolutions/s] P : float Actual power required to mix, ignoring mechanical inefficiencies [W] T : float Tank diameter, [m] H : float Tank height, [m] mu : float Mixture viscosity, [Pa*s] rho : float Mixture density, [kg/m^3] D : float, optional Impeller diameter [m] homogeneity : float, optional Fraction completion of mixing, [] Returns ------- t : float Time for specified degree of homogeneity [s] Notes ----- If impeller diameter is not specified, assumed to be 0.5 tank diameters. The first example is solved forward rather than backwards here. A rather different result is obtained, but is accurate. No check to see if the mixture if laminar is currently implemented. This would under predict the required time. Examples -------- >>> agitator_time_homogeneous(D=36*.0254, N=56/60., P=957., T=1.83, H=1.83, mu=0.018, rho=1020, homogeneity=.995) 15.143198226374668 >>> agitator_time_homogeneous(D=1, N=125/60., P=298., T=3, H=2.5, mu=.5, rho=980, homogeneity=.95) 67.7575069865228 References ---------- .. [1] Paul, Edward L, Victor A Atiemo-Obeng, and Suzanne M Kresta. Handbook of Industrial Mixing: Science and Practice. Hoboken, N.J.: Wiley-Interscience, 2004. ''' if not D: D = T*0.5 Np = P*g/rho/N**3/D**5 Re_imp = rho/mu*D**2*N regime_constant = Np**(1/3.)*Re_imp if regime_constant >= min_regime_constant_for_turbulent: Fo = (5.2/regime_constant) else: Fo = (183./regime_constant)**2 time = rho*T**1.5*sqrt(H)/mu*Fo multiplier = adjust_homogeneity(homogeneity) return time*multiplier
[docs]def Kp_helical_ribbon_Rieger(D, h, nb, pitch, width, T): r'''Calculates product of power number and Reynolds number for a specified geometry for a heilical ribbon mixer in the laminar regime. One of several correlations listed in [1]_, it used more data than other listed correlations and was recommended. .. math:: K_p = 82.8\frac{h}{D}\left(\frac{c}{D}\right)^{-0.38} \left(\frac{p}{D}\right)^{-0.35} \left(\frac{w}{D}\right)^{0.20} n_b^{0.78} Parameters ---------- D : float Impeller diameter [m] h : float Ribbon mixer height, [m] nb : float: Number of blades, [-] pitch : float Height of one turn around a helix [m] width : float Width of one blade [m] T : float Tank diameter, [m] Returns ------- Kp : float Product of Power number and Reynolds number for laminar regime [] Notes ----- Example is from example 9-6 in [1]_. Confirmed. Examples -------- >>> Kp_helical_ribbon_Rieger(D=1.9, h=1.9, nb=2, pitch=1.9, width=.19, T=2) 357.39749163259256 References ---------- .. [1] Paul, Edward L, Victor A Atiemo-Obeng, and Suzanne M Kresta. Handbook of Industrial Mixing: Science and Practice. Hoboken, N.J.: Wiley-Interscience, 2004. .. [2] Rieger, F., V. Novak, and D. Havelkov (1988). The influence of the geometrical shape on the power requirements of ribbon impellers, Int. Chem. Eng., 28, 376-383. ''' c = 0.5*(T - D) return 82.8*h/D*(c/D)**-.38*(pitch/D)**-0.35*(width/D)**0.2*nb**0.78
[docs]def time_helical_ribbon_Grenville(Kp, N): r'''Calculates product of time required for mixing in a helical ribbon coil in the laminar regime according to the Grenville [2]_ method recommended in [1]_. .. math:: t = 896\times10^3K_p^{-1.69}/N Parameters ---------- Kp : float Product of power number and Reynolds number for laminar regime [] N : float Speed of impeller, [revolutions/s] Returns ------- t : float Time for homogeneity [s] Notes ----- Degree of homogeneity is not specified. Example is from example 9-6 in [1]_. Confirmed. Examples -------- >>> time_helical_ribbon_Grenville(357.4, 4/60.) 650.980654028894 References ---------- .. [1] Paul, Edward L, Victor A Atiemo-Obeng, and Suzanne M Kresta. Handbook of Industrial Mixing: Science and Practice. Hoboken, N.J.: Wiley-Interscience, 2004. .. [2] Grenville, R. K., T. M. Hutchinson, and R. W. Higbee (2001). Optimisation of helical ribbon geometry for blending in the laminar regime, presented at MIXING XVIII, NAMF. ''' return 896E3*Kp**-1.69/N
### Tee mixer
[docs]def size_tee(Q1, Q2, D, D2, n=1, pipe_diameters=5): r'''Calculates CoV of an optimal or specified tee for mixing at a tee according to [1]_. Assumes turbulent flow. The smaller stream in injected into the main pipe, which continues straight. COV calculation is according to [2]_. Parameters ---------- Q1 : float Volumetric flow rate of larger stream [m^3/s] Q2 : float Volumetric flow rate of smaller stream [m^3/s] D : float Diameter of pipe after tee [m] D2 : float Diameter of mixing inlet, optional (optimally calculated if not specified) [m] n : float Number of jets, 1 to 4 [] pipe_diameters : float Number of diameters along tail pipe for CoV calculation, 0 to 5 [] Returns ------- CoV : float Standard deviation of dimensionless concentration [-] Notes ----- Not specified if this works for liquid also, though probably not. Example is from example Example 9-6 in [1]_. Low precision used in example. Examples -------- >>> size_tee(Q1=11.7, Q2=2.74, D=0.762, D2=None, n=1, pipe_diameters=5) 0.2940930233038544 References ---------- .. [1] Paul, Edward L, Victor A Atiemo-Obeng, and Suzanne M Kresta. Handbook of Industrial Mixing: Science and Practice. Hoboken, N.J.: Wiley-Interscience, 2004. .. [2] Giorges, Aklilu T. G., Larry J. Forney, and Xiaodong Wang. "Numerical Study of Multi-Jet Mixing." Chemical Engineering Research and Design, Fluid Flow, 79, no. 5 (July 2001): 515-22. doi:10.1205/02638760152424280. ''' V1 = Q1/(pi/4*D**2) # Cv = Q2/(Q1 + Q2) # COV0 = sqrt((1-Cv)/Cv) if D2 is None: D2 = (Q2/Q1)**(2/3.)*D V2 = Q2/(pi/4*D2**2) B = n**2*(D2/D)**2*(V2/V1)**2 if not n == 1 and not n == 2 and not n == 3 and not n ==4: raise ValueError('Only 1 or 4 side streams investigated') if n == 1: if B < 0.7: E = 1.33 else: E = 1/33. + 0.95*log(B/0.7) elif n == 2: if B < 0.8: E = 1.44 else: E = 1.44 + 0.95*log(B/0.8)**1.5 elif n == 3: if B < 0.8: E = 1.75 else: E = 1.75 + 0.95*log(B/0.8)**1.8 else: if B < 2: E = 1.97 else: E = 1.97 + 0.95*log(B/2.)**2 COV = sqrt(0.32/B**0.86*(pipe_diameters)**-E) return COV
### Commercial motionless mixers """Data from: Paul, Edward L, Victor A Atiemo-Obeng, and Suzanne M Kresta. Handbook of Industrial Mixing: Science and Practice. Hoboken, N.J.: Wiley-Interscience, 2004.""" StatixMixers = {} StatixMixers['KMS'] = {'Name': 'KMS', 'Vendor': 'Chemineer', 'Description': 'Twisted ribbon. Alternating left and right twists.', 'KL': 6.9, 'KiL': 0.87, 'KT': 150, 'KiT': 0.5} StatixMixers['SMX'] = {'Name': 'SMX', 'Vendor': 'Koch-Glitsch', 'Description': 'Guide vanes 45 degrees to pipe axis. Adjacent elements rotated 90 degrees.', 'KL': 37.5, 'KiL': 0.63, 'KT': 500, 'KiT': 0.46} StatixMixers['SMXL'] = {'Name': 'SMXL', 'Vendor': 'Koch-Glitsch', 'Description': 'Similar to SMX, but intersection bars at 30 degrees to pipe axis.', 'KL': 7.8, 'KiL': 0.85, 'KT': 100, 'KiT': 0.87} StatixMixers['SMF'] = {'Name': 'SMF', 'Vendor': 'Koch-Glitsch', 'Description': 'Three guide vanes projecting from the tube wall in a way as to not contact. Designed for applications subject to plugging.', 'KL': 5.6, 'KiL': 0.83, 'KT': 130, 'KiT': 0.4}
[docs]def COV_motionless_mixer(Ki, Q1, Q2, pipe_diameters): r'''Calculates CoV of a motionless mixer with a regression parameter in [1]_ and originally in [2]_. .. math:: \frac{CoV}{CoV_0} = K_i^{L/D} Parameters ---------- Ki : float Correlation parameter specific to a mixer's design, [-] Q1 : float Volumetric flow rate of larger stream [m^3/s] Q2 : float Volumetric flow rate of smaller stream [m^3/s] pipe_diameters : float Number of diameters along tail pipe for CoV calculation, 0 to 5 [] Returns ------- CoV : float Standard deviation of dimensionless concentration [-] Notes ----- Example 7-8.3.2 in [1]_, solved backwards. Examples -------- >>> COV_motionless_mixer(Ki=.33, Q1=11.7, Q2=2.74, pipe_diameters=4.74/.762) 0.0020900028665727685 References ---------- .. [1] Paul, Edward L, Victor A Atiemo-Obeng, and Suzanne M Kresta. Handbook of Industrial Mixing: Science and Practice. Hoboken, N.J.: Wiley-Interscience, 2004. .. [2] Streiff, F. A., S. Jaffer, and G. Schneider (1999). Design and application of motionless mixer technology, Proc. ISMIP3, Osaka, pp. 107-114. ''' Cv = Q2/(Q1 + Q2) COV0 = sqrt((1-Cv)/Cv) COVr = Ki**(pipe_diameters) COV = COV0*COVr return COV
[docs]def K_motionless_mixer(K, L, D, fd): r'''Calculates loss coefficient of a motionless mixer with a regression parameter in [1]_ and originally in [2]_. .. math:: K = K_{L/T}f\frac{L}{D} Parameters ---------- K : float Correlation parameter specific to a mixer's design, [-] Also specific to laminar or turbulent regime. L : float Length of the motionless mixer [m] D : float Diameter of pipe [m] fd : float Darcy friction factor [-] Returns ------- K : float Loss coefficient of mixer [-] Notes ----- Related to example 7-8.3.2 in [1]_. Examples -------- >>> K_motionless_mixer(K=150, L=.762*5, D=.762, fd=.01) 7.5 References ---------- .. [1] Paul, Edward L, Victor A Atiemo-Obeng, and Suzanne M Kresta. Handbook of Industrial Mixing: Science and Practice. Hoboken, N.J.: Wiley-Interscience, 2004. .. [2] Streiff, F. A., S. Jaffer, and G. Schneider (1999). Design and application of motionless mixer technology, Proc. ISMIP3, Osaka, pp. 107-114. ''' return L/D*fd*K