Stoodley P, Lewandowski Z, Boyle J D, Lappin-Scott H M
Environmental Microbiology Research Group, University of Exeter, Department of Biological Sciences, Hatherly Laboratories, Exeter, Devon EX4 4PS, United
Biotechnol Bioeng. 1998 Mar 5;57(5):536-44. doi: 10.1002/(sici)1097-0290(19980305)57:5<536::aid-bit5>3.0.co;2-h.
Mixed population biofilms consisting of Pseudomonas aeruginosa, P. fluorescens, and Klebsiella pneumoniae were grown in a flow cell under turbulent conditions with a water flow velocity of 18 cm/s (Reynolds number, Re, =1192). After 7 days the biofilms were patchy and consisted of cell clusters and streamers (filamentous structures attached to the downstream edge of the clusters) separated by interstitial channels. The cell clusters ranged in size from 25 to 750 microm in diameter. The largest clusters were approximately 85 microm thick. The streamers, which were up to 3 mm long, oscillated laterally in the flow. The motion of the streamers was recorded at various flow velocities up to 50.5 cm/s (Re 3351) using confocal scanning laser microscopy. The resulting time traces were evaluated by image analysis and fast Fourier transform analysis (FFT). The amplitude of the motion increased with flow velocity in a sigmoidal shaped curve, reaching a plateau at an average fluid flow velocity of approximately 25 cm/s (Re 1656). The motion of the streamers was possibly limited by the flexibility of the biofilm material. FFT indicated that the frequency of oscillation was directly proportional to the average flow velocity (u(ave)) below 9.5 cm/s (Re 629). At u(ave) greater than 9.5 cm/s, oscillation frequencies were above our measurable frequency range (0.12-6.7 Hz). The oscillation frequency was related to the flow velocity by the Strouhal relationship, suggesting that the oscillations were possibly caused by vortex shedding from the upstream biofilm clusters. A loss coefficient (k) was used to assess the influence of biofilm accumulation on pressure drop. The k across the flow cell colonized with biofilm was 2.2 times greater than the k across a clean flow cell.
由铜绿假单胞菌、荧光假单胞菌和肺炎克雷伯菌组成的混合菌群生物膜在流动池中以18厘米/秒的水流速度(雷诺数Re = 1192)在湍流条件下生长。7天后,生物膜呈斑块状,由细胞簇和菌缕(附着在细胞簇下游边缘的丝状结构)组成,中间由间隙通道隔开。细胞簇的直径大小在25至750微米之间。最大的细胞簇厚度约为85微米。长达3毫米的菌缕在水流中横向摆动。使用共聚焦扫描激光显微镜在高达50.5厘米/秒(Re 3351)的不同流速下记录菌缕的运动。通过图像分析和快速傅里叶变换分析(FFT)对所得的时间轨迹进行评估。运动幅度随流速呈S形曲线增加,在平均流体流速约为25厘米/秒(Re 1656)时达到平稳状态。菌缕的运动可能受到生物膜材料柔韧性的限制。FFT表明,在9.5厘米/秒(Re 629)以下,振荡频率与平均流速(u(ave))成正比。在u(ave)大于9.5厘米/秒时,振荡频率超出了我们的可测量频率范围(0.12 - 6.7赫兹)。振荡频率通过斯特劳哈尔关系与流速相关,这表明振荡可能是由上游生物膜簇的涡旋脱落引起的。使用损失系数(k)来评估生物膜积累对压降的影响。生物膜定植的流动池中的k比清洁流动池中的k大2.2倍。