DOI: 10.17077/etd.78yn0isg
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Thermal deactivation of Pseudomonas aeruginosa biofilms

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Cited by 9 publications
(22 citation statements)
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“…The drip flow reactor has been shown to be a good model for growing large, bacterial dense, biofilms. 120 This was in comparison to other growth means, such as the shaker plate biofilm, explored more in Chapter 5, which had lower density biofilms than the drip flow reactor-grown biofilms. It was discovered early on that in order to quantify the amount of bacterial death observed a very high number of bacteria was required to accurately report the reduction.…”
Section: These Experiments Provide a Better Understanding Of Biofilmsmentioning
confidence: 93%
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“…The drip flow reactor has been shown to be a good model for growing large, bacterial dense, biofilms. 120 This was in comparison to other growth means, such as the shaker plate biofilm, explored more in Chapter 5, which had lower density biofilms than the drip flow reactor-grown biofilms. It was discovered early on that in order to quantify the amount of bacterial death observed a very high number of bacteria was required to accurately report the reduction.…”
Section: These Experiments Provide a Better Understanding Of Biofilmsmentioning
confidence: 93%
“…Biofilms cultured in drip flow reactors were thicker (50-150 µm) and more carpetlike, as shown in Figure 3.2, than biofilms grown in shaker plates. 121…”
Section: Drip Flow Reactor Biofilmsmentioning
confidence: 99%
“…To investigate the effect heat treatment has on biofilms, P. aeruginosa biofilms have been thermally shocked at medically accessible times and temperatures ranging from 1 min to 30 min and from 37 °C to 80 °C. 27 In that study, the thermal load was provided by a temperature controlled water bath and demonstrated up to six orders of magnitude reduction in colony forming units (CFUs) per cm 2 2. Thermal deactivation of biofilms using a water bath heat shock method.…”
Section: Thermal Deactivationmentioning
confidence: 99%
“…If (time.eq.1.or.mod(time,int((ttotal/60/delt))).eq.0) Then Do k=z2+1,z3 qz(k-z2)=(3.0*T(imax/2,y2+1,k)-4.0* T(imax/2,y2+2,k) & +T(imax/2,y2+3,k))*kcon(imax/2,y2+1,k)/2.0/dely/10000.0 End Do write(4,40)time*delt,qz(1), qz(2), qz(3), qz(4), qz (5), & qz (6), qz (7), qz (8), qz(9), qz(10), & qz (11), qz (12), qz (13), qz (14),qz (15), & qz (16), qz (17), qz (18), qz (19),qz (20), & qz (21), qz (22), qz (23), qz(24),qz (25), & qz (26), qz (27), qz (28), qz (29),qz (30), & qz (31), qz (32), qz (33), qz (34),qz (35), & qz (36), qz (37), qz (38), qz 39 Do k=5,kmax-4,2 rhoustar(imax-1,j,k)=rhoustar(imax-3,j,k) End Do End Do Do j=3,jmax-2,2 Do k=3,kmax-2,2 rhovstar(imax,j,k)=rhovstar(imax-2,j,k) End Do End Do Do j=4,jmax-3,2 Do k=4,kmax-3,2 rhowstar(imax-1,j,k)=rhowstar(imax-3,j,k) End Do End Do !using rhoustar, rhovstar, rhowstar, solve for the corrected pressure ! (denoted as pp)using the pressure correction formula which is solved !using the successive overrelaxation subroutine (sor) !prepare e matrix for sor subroutine !e can be thought of as a mass source term and represents how far the !continuity equation deviates from the converged answer.…”
Section: Expanding the Computational Modelmentioning
confidence: 99%
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