E. coli Cultivation in a 12L and 120L CELL-tainer™ Single-Use Bioreactor
Although single-use bioreactors are widely applied in the biopharmaceutical industry, microbial cultivation in them is restricted due to limitations in oxygen mass transfer, mixing, and heat transfer. The CELL-tainer™ single-use bioreactor makes use of an innovative principle applying a two-dimensional (2D) rocking motion, thus providing excellent mass transfer, making this single-use reactor very suitable for microbial cultivation at different scales. With a simple pillow-shaped bag without moving parts, the technology is robust and leads to cost savings compared with other single-use or classical glass or stirred bioreactors.
Mass Transfer
In a CELL-tainer single-use bioreactor, a pillow-shaped bag is positioned in a tray. The movement of this tray is in two directions: a vertical rocking motion combined with a horizontal translation. This combination of movement results in oxygen mass transfer coefficients, kLa > 300 (h−1) both at 12L and 120L scales (working volumes). The oxygen mass transfer coefficients have been determined by using the dynamic method (Figure 1).
Figure 1: ()
With aeration by air, an oxygen mass transfer (OTR) of at least 100 (mmolh−1) can be achieved. As a function of the rocking speed, mixing times have been measured to be 12–16 seconds at a working volume of 12L in the 20L CELL-tainer and 60–120 seconds at a working volume of 115L in the 200L CELL-tainer.
Figure 2: ()
Scale-Up of the Cell-tainer Single-Use Bioreactor
In order to keep the fluid characteristics the same at different scales, the ratio of rocking angle (including horizontal displacement) and the length of the bag have been kept comparable at different scales such that the oxygen mass transfer coefficient will be in the same range at both scales (Figure 1). It is obvious that the kLa is strongly dependent on the liquid volume, as the kLa is a volume dependent parameter. Due to the principle of surface aeration applied and as the liquid depth also changes with volume, the shape of the wave is strongly influenced by filling volume, resulting in a volume dependent entrapment of air into the liquid.