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Articles; Pharmaceutical Biotechnology

Effect of hydrophilic polymers on the wettability, static and dynamic, of solid substrate covered by confluent monolayer of air-damaged SIRC cells

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Pages 390-394 | Received 20 Mar 2014, Accepted 08 Dec 2014, Published online: 13 Jan 2015

Figures & data

Table 1. Main characteristics of polymers.

Figure 1. Dependence of the equilibrium contact angle (θ) between static air bubble and solid surface covered with air-damaged SIRC on polymer concentration. Zero per cent polymer concentration corresponds to control, i.e. pure saline solution with no polymer dissolved.

Figure 1. Dependence of the equilibrium contact angle (θ) between static air bubble and solid surface covered with air-damaged SIRC on polymer concentration. Zero per cent polymer concentration corresponds to control, i.e. pure saline solution with no polymer dissolved.

Figure 2. Dependence of the advancing contact angle (θ) between air bubble at contraction and solid surface covered with air-damaged SIRC on polymer concentration. Zero per cent polymer concentration corresponds to control, i.e. pure saline solution with no polymer dissolved.

Figure 2. Dependence of the advancing contact angle (θ) between air bubble at contraction and solid surface covered with air-damaged SIRC on polymer concentration. Zero per cent polymer concentration corresponds to control, i.e. pure saline solution with no polymer dissolved.

Figure 3. Dependence of the receding contact angle between air bubble at expansion and solid surface covered with air-damaged SIRC on polymer concentration. Zero per cent polymer concentration corresponds to control, i.e. pure saline solution with no polymer dissolved.

Figure 3. Dependence of the receding contact angle between air bubble at expansion and solid surface covered with air-damaged SIRC on polymer concentration. Zero per cent polymer concentration corresponds to control, i.e. pure saline solution with no polymer dissolved.

Table 2. Dependence of the average contact angle on the polymers concentration.

Figure 4. Dependence of the advancing contact angle (θ) on the distance travelled by the bubble edge (R) over the cell covered surface of the solid support for each polymer concentration: HEC (A), HPMC (B), PO12 (C), SCS (D).

Figure 4. Dependence of the advancing contact angle (θ) on the distance travelled by the bubble edge (R) over the cell covered surface of the solid support for each polymer concentration: HEC (A), HPMC (B), PO12 (C), SCS (D).

Figure 5. Dependence of the receding contact angle (θ) on the distance travelled by the bubble edge (R) over the cell covered surface of the solid support for each polymer concentration: HEC (A), HPMC (B), PO12 (C), SCS (D).

Figure 5. Dependence of the receding contact angle (θ) on the distance travelled by the bubble edge (R) over the cell covered surface of the solid support for each polymer concentration: HEC (A), HPMC (B), PO12 (C), SCS (D).