A study of mixing by PIV and PLIF in bioreactor of animal cell culture

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Sixth International Symposium on Mixing in Industrial Process Industries ISMIP VI Niagara on the Lake, Niagara Falls, Ontario, Canada August 17-21, 2008 A study of mixing by PIV and PLIF in bioreactor of animal cell culture M-L Collignon 1, M.Crine 1, J-F Chaubard 2, L.Peeters 2, S.Dessoy 2, D.Toye 1 1 Laboratory of Chemical Engineering, Liege University, Belgium 2 GlaxoSmithKline Biologicals, Rixensart, Belgium

Collaboration between: Background of the research the Laboratory of Chemical Engineering of Liege University the Company GlaxoSmithKline Biologicals Process development of a animal cell culture on microcarrier in a stirred tank used for vaccine production

Introduction Positive effect of mixing : Keeping in complete suspension the microcarriers (N>Njs) Homogenization of the culture medium Negative effect of mixing: Creation of mechanical constraints micro-shearing collision

Goals of the research Productivity of cell culture Local cell environment Mixing conditions: agitator design tank design rotating speed Experimental characterization of the local cell environment depending on the mixing conditions The choice of optimal agitation conditions to have: microcarrier in suspension, small concentration gradient small mechanical constraints

Materials and methods 20 L standard tank : d 6 axial impellers : Propeller TTP (Mixel) d = 0.125 or 0.150 m (TTP125) (TTP150) Propeller 3 streamed blades (VMI) d=0.160 m (3SB 160) Propeller A315 (Lightnin) d=0.125 or 0.150 m (A315125) (A315150) Propeller A310 (Lightnin) d=0.156 m (A310 156)

Materials and methods Characterisation of local cell environment by P.I.V. and P.L.I.F. apparatus (Dantec Dynamics S.A., Denmark) P.I.V. tracer: polyamide particles, (20 µm, 1.03g/cm³) P.L.I.F. tracer: 5ml of 8 mg/l fluorescent Rhodamine 6G Injection position: Along the wall tank and same height than the impeller Camera Hi/Sense P.I.V/P.L.I.F: sensors CCD, 1280x1024 pixels Lens AF Micro Nikkor 60 mm F2.8D (Nikon) Laser Solo II-30 (New Wave Gemini): Nd-Yag, double cavity, 2X30 MJ, 532 nm Processor Correlator 2500 (Dantec Dynamics) Software FlowManager 4.71 (Dantec Dynamics)

Materials and methods Exploitation of P.I.V. measurements: impeller A315 150 at 38 rpm Time average macro-shearing field (s -1 ) computed by Time average velocity field (m.s 1 ) for a half tank U x z + U x z

Materials and methods Exploitation of P.I.V. measurements: Kolmogorov scale field Fluctuation velocity field : 2 2 2 u' r u' z u' r r z z 2 u' z u' r u' z r z dr 2 + 2 + 3 ε= υ u ' = u U Local rate of energy dissipation : + 3 + 2 Kolmogorov scale field : λ= 1 4 υ 3 ε

Materials and methods Exploitation of P.L.I.F. measurements: a global mixing time of 95% homogeneity by log variance method (Brown & al, 2004, Handbook of Industrial mixing, Science and Practice, 145-256, John Wiley&Sons Inc.) 0-0.5-1 1 R G G G G 2 i 0 log = log 1 σ 0 2 4 6 8 10 12 14 16 18 20 0 2 log (variance) mixing time 95% log (variance) -1.5-2 -2.5-3 -3.5-4 time (s)

Results Results division in two parts: 1. Impellers comparison at the just-suspended rotating speed Njs 2. Impellers comparison as function of the evolution of their hydrodynamic quantities while the rotating speed increases

Impeller comparison at N js Interest? 1 st agitation goal : keeping microcarriers in complete suspension Impellers comparison at the same conditions regarding to microcarrier suspension Results: A315 150 TTP 150 A310 156 TTP 125 3SB 160 A315 125 N js (rpm) 38 40 49 50 53 54 3SD A310 TTP A315

Impeller comparison at N js Time average velocity field : N js (rpm) V average (m.s -1 ) V 90% (m.s -1 ) A315 150 38 0.029 0.055 TTP 150 40 0.030 0.055 A310 156 49 0.031 0.06 TTP 125 50 0.027 0.050 3SB 160 53 0.032 0.065 A315 125 54 0.030 0.06 Same hydrodynamic pattern average and maximum velocity values very close to each other A315 150 at 38 rpm

Macro-shearing distributions : Impeller Comparison at N js Calculated by: U x z + U z x Comparison criterion Similar approaches available in the literature (Croughan & al, 1987; Hu,1983; Sinskey & al, 1981) A315 150 at 38 rpm TTP 125 at 50 rpm TTP 125 A310 156 TTP 150 A315 150 3SB 160 A315 125 cis average (s -1 ) cis 90% (s -1 ) 1.299 3 < 1.387 < 1.437 < 1.485 < 1.541 < 3.4 3.4 3.6 3.6 1.609 4.2 TTP 125 creates the smallest macro-shearing

Impeller comparison at N js Rate of energy dissipation and Kolmogorov scale : Gradients situated outside the measurement plane estimated by supposing an isotropic turbulence 2 2 2 2 r z r z r z u u u u u u εmin= υ 2 2 3 3 2 r + z + z + r + z dr But under-estimation of local rate of energy dissipation if PIV resolution > kolmorogov scale (Baldi & al, 2002, On the measurement of turbulence energy dissipation in stirred vessels with PIV techniques, Proceedings of the 11th International Symposium on Applied Laser Techniques in Fluid Mechanic,Lisbon, Portugal, July 8-11). Over-estimation of kolmogorov scale λ k max 1 3 4 υ = ε min

Impeller comparison at N js Kolmogorov scale distribution : Microcarrier Size (250 µm) Microcarrier Size (250 µm) A315 150 à 38 rpm TTP 125 à 50 rpm Relative size of the area (%) where λ d microcarrier TTP 125 0.90 A310 156 TTP 150 3SB 160 < < < A315 150 < < 1.45 1.97 3.48 3.72 A315 125 5.16 TTP 125 creates the smallest area where the micro-shearing could be high

Impeller comparison at N js Characterization of the constraints created by collisions: Based on Cherry et Papoutsakis model (1989): Turbulent Collision Severity [ ] TCS W = in teractio n freq u ency k in etic en erg y o f th e in teractio n [ J ] vo lu m e -3 m icro carrier concen tratio n m Impeller Collision Severity s -1 m 3 TCS s 3 2 2 5 π ρs d p εs P V = µ 72 kinetic energy ICS = reactor volume (window area)(velocity past blade) Classification : 4 9 π ρs nb N ICS= 512 V 3 d 4 d 4 P TCS ICS TTP 125 < TTP 150 < 3SB 160 < A310 156 < A315 125 < A315 150 TTP 125 < TTP 150 < A315 150 < A315 125 < A310 156 < 3SB 160 TTP 125 creates the smallest mechanical constraints due to collisions

Impellers Comparison at N js Mixing time: Obtained from P.L.I.F measurements : Mixing time (s) 3SB 160 18 A315 150 A310 156 A315 125 TTP 150 < < < < < 20 22 23 23 TTP 125 33 TTP 125 creates the highest mixing time But small in comparison to the response time of cell metabolism to a perturbation of their environment ~ 1 hour

Impellers Comparison at N js Conclusion on the impeller comparison at Njs Choice of the impeller TTP 125 in view of its characteristics : the smallest macro-shearing; the smallest area where micro-shearing could be high; the smallest mechanical constraints due to collisions; the highest mixing time but small in comparison to the response time of cell metabolism.

Results Results division in two parts: 1. Impellers comparison at the just-suspended rotating speed Njs 2. Impellers comparison as function of the evolution of their hydrodynamic quantities while the rotating speed increases

Variation of quantities as function of N Interest? Formation of 3 beads agglomerate on average during the cell culture (Cherry & Papoutsakis, 1988) Aeration not taken into account N js insufficient Interest of knowing the quantity variations with the rotating speed

Variation of quantities as function of N Macro-shearing distribution (s -1 ) : 14 12 10 8 6 4 2 0.1143 0.0943 0.08 0.0799 0.0771 0.0715 0,0442 0,0381 0,0313 0,0309 0,0303 0,0262 A315 125 90 pc A315 150 90 pc A310 156 90 pc TTP 125 90 pc TTP 150 90 pc 3SB 160 90 pc A315 125 average A315 150 average A310 156 average TTP 125 average TTP 150 average 3SB 160 average 0 40 60 80 100 120 140 rotating speed (rpm) Linear evolution with the impeller rotating speed Smallest increase (slope of the straight line) associated to the impeller TTP 125

Variation of quantities as function of N Micro-shearing : relative size of the area where microshearing is intensive (%) 1 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 A315 125 A315 150 A310 156 TTP 125 TTP 150 3SB 160 0 20 40 60 80 100 120 140 rotating speed (rpm) Smallest increase of the area where the micro-shearing could be high associated to the impeller TTP 125

Variation of quantities as function of N Mechanical constraints due to collisions : in c r e a s in g o f IC S b e tw e e n tw o r o ta tin g s p e e d s 1,2E-13 1E-13 8E-14 6E-14 4E-14 2E-14 0 A315 125 A315 150 A310 156 TTP 125 TTP 150 3SB 160 60 70 80 90 100 110 120 130 rotating speed (rpm) In c r e a s in g o f T C S s b e tw e e n tw o r o ta tin g s p e e d s 1,6E-05 1,4E-05 1,2E-05 1,0E-05 8,0E-06 6,0E-06 4,0E-06 2,0E-06 0,0E+00 A315 125 A315 150 A310 156 TTP 125 TTP 150 3SD 160 60 70 80 90 100 110 120 130 rotating speed (rpm) Smallest increase of mechanical constraints associated to the impeller TTP 125

Mixing time: Variation of quantities as function of N macroscopic mixing time (s) 35 30 25 20 15 10 5 A315 125 A315 150 A310 156 TTP 125 TTP 150 3SB 160 0 0 20 40 60 80 100 120 140 rotating speed (rpm) Highest decrease associated at the impeller TTP 125

Variation of quantities as function of N Conclusions on that part of the results Favourable evolution of hydrodynamic quantities of the impeller TTP 125 : Smallest increase of macro-shearing Smallest increase of micro-shearing Smallest increase of mechanical constraints due to collisions Highest decrease of mixing time

In summary: Conclusions Goals : 1) Study the influence of agitation conditions on cell local environment 2) Determine the optimal agitation conditions Tools Use of P.I.V. and P.L.I.F. techniques to compare 6 impellers Results 1) Impellers comparison at Njs Choice of the impeller TTP 125: smallest mechanical constraints mixing time < metabolism response time 2) Impellers comparison when the rotating speed increases Choice of the impeller TTP 125: smallest increase of mechanical constraints highest decrease of mixing time

Conclusions Goals achieved regarding to impeller selection not achieved regarding to rotating speed choice Futures: Improvement of the knowledge on animal cell behaviour 1. Determination of the animal cell resistance to hydrodynamic constraints 2. Experiment these agitation conditions on animal cell cultures Improvement of measurement techniques 1. Use of 3-D PIV to obtain the 3 rd velocity component 2. Refining the Kolmogorov scale measurements

Acknowledgements I m grateful to FNRS ( National Fund for Scientific Research, Belgium) for a grant of Research Fellow I thank the society GlaxoSmithKline Biologicals for the fruitful collaboration Thank you for your attention