2.1. Membrane Morphology
Figure 1 shows cross-sectional structure of the seven-channel Al
2O
3-YSZ capillary membrane sintered at 1400 °C. The membrane has a symmetric macrostructure with six channels distributing evenly around the central channel. The outer diameter is 3.2 mm and the inner diameter of each channel is around 1.0 mm. The walls between channels are composed of micro-channels and densely packed sponge-like regions. At the walls next to the outer surface, similar features are also present, but the micro-channels from the outer surface are much shorter than the micro-channels from the inner surfaces. The generation of micro-channels is due to interfacial instability and has been well explained elsewhere [
10]. Closer examination on the microstructure of the cross section at the sponge-like part reveals the porous structure of the sintered sample, in which necks between ceramic grains can be clearly seen, indicating that proper sintering has been reached at 1400 °C.
Figure 2 shows SEM images of the sintered membrane. Obviously, the outer surface was smoother than the inner surface, due to the fact that a short air gap was used during the spinning process, which gives a relaxation time for the outer surface to ease the disturbance produced by the spinneret. However, this relaxation was not possible at the inner surface, thus leading to the rougher surface (
Figure 2a,b). By increasing the sintering temperature to 1450 °C, similar results were observed (
Figure 2c,d), but both surfaces were much denser than the sample sintered at 1400 °C, leaving much fewer pores on the surfaces.
Figure 1.
Microstructure of the Al2O3-YSZ seven-channel capillary membrane sintered at 1400 °C: (a) whole view of the cross section; (b) cross-sectional view of the internal wall between channels; (c) cross-sectional view of the outer wall and (d) micro-structure in the sponge-like region.
Figure 1.
Microstructure of the Al2O3-YSZ seven-channel capillary membrane sintered at 1400 °C: (a) whole view of the cross section; (b) cross-sectional view of the internal wall between channels; (c) cross-sectional view of the outer wall and (d) micro-structure in the sponge-like region.
Figure 2.
Outer and inner surface SEM images of the Al2O3-YSZ seven-channel capillary membranes sintered at 1400 and 1450 °C. (a) outer surface of the 1400 °C sample; (b) inner surface of the 1400 °C sample; (c) outer surface of the 1450 °C sample and (d) inner surface of the 1400 °C sample.
Figure 2.
Outer and inner surface SEM images of the Al2O3-YSZ seven-channel capillary membranes sintered at 1400 and 1450 °C. (a) outer surface of the 1400 °C sample; (b) inner surface of the 1400 °C sample; (c) outer surface of the 1450 °C sample and (d) inner surface of the 1400 °C sample.
2.2. Mechanical Property
The sintering temperature affects the mechanical property, as expected.
Figure 3 gives three-point bending results of the reinforced Al
2O
3-YSZ capillary membranes. The results are similar to those of pure alumina seven-channel capillary tubes [
8]. It is interesting to note that at a sintering temperature lower than 1430 °C, the fracture load of the Al
2O
3-YSZ tube is in fact lower than the pure alumina tube, but it is increased quickly as the sintering temperature is increased. This behavior indicates a change in the sintering mechanism that might occur when the Al
2O
3-YSZ tube was sintered at a temperature higher than 1430 °C. The change in sintering mechanisms at higher sintering temperatures is also reflected by the pore structure, which will be discussed later.
Figure 3.
Three point bending fracture load of the Al
2O
3-YSZ and pure alumina membranes [
8].
Figure 3.
Three point bending fracture load of the Al
2O
3-YSZ and pure alumina membranes [
8].
Figure 4 shows force-extension curves of the Al
2O
3-YSZ seven-channel capillary tube sintered at 1440 °C and a pure alumina seven-channel tube sintered at 1450 °C. Although these two tubes have very close fracture loads (22.85 N for Al
2O
3-YSZ
vs. 21.52 N for pure alumina), their bending extensions at the breaking point are quite different. The Al
2O
3-YSZ tube could extend 68.3% more than the pure alumina tube, meaning that it can adsorb 78.7% more energy than the pure alumina tube before breaking if the tube undergoes a continuous impact. In addition, if the tubes are subject to pulsed impacts where the actual force produced is affected by the initial momentum and the acting time, the Al
2O
3-YSZ tube would be more advantageous, because it can prolong the acting time and thus help to reduce the actual force on it.
Figure 4.
Extension-force bending curves of the Al2O3-YSZ and pure alumina seven-channel capillary membranes.
Figure 4.
Extension-force bending curves of the Al2O3-YSZ and pure alumina seven-channel capillary membranes.
2.3. Pore Size and Water Permeation
The size of open pores and their size distribution of the Al
2O
3-YSZ membranes sintered at 1400–1450 °C were measured by using the gas-liquid displacement method. The mean flow pore size of all samples is in the range of 210–240 nm, which is not significantly affected by the sintering temperature. However, the pore size distribution (
Figure 5) shows a turning from a singular distribution to a binary distribution when the sintering temperature is elevated from 1400 to above 1430 °C. For the sample sintered at 1400 °C, only one peak at 235 nm with a percent flow of 86% can be seen,
i.e., a very narrow pore size distribution. However, for the sample sintered at 1430 °C, two peaks at 240 and 216 nm are observed. Similarly, for the sample sintered at 1440 °C, the two peaks are at 244 and 212 nm. For the sample sintered at 1450 °C, the two peaks merge into a broad peak, and the mean flow pore size shifts to 215 nm. The change in the pore size distribution is concurrent with the change in mechanical property, corresponding a subtle change of the sintering behavior.
Figure 5.
Gas-liquid-displacement pore size distributions of the Al2O3-YSZ membranes sintered at different temperatures.
Figure 5.
Gas-liquid-displacement pore size distributions of the Al2O3-YSZ membranes sintered at different temperatures.
The pore size distribution inside the sample sintered at 1440 °C was also determined by mercury porosimetry, as shown in
Figure 6. The mercury porosimetry result shows a single narrow peak at 230 nm, identical to the mean flow pore size determined by the gas-liquid displacement. This result implies that the effective transport path in this membrane is the inter-granule pores in the sponge-like region, which is not affected by the micro-channels present in the membrane. The binary distribution of the pore structure obtained by the gas-liquid displacement was not observed when using mercury porosimetry, which is likely due to the natural difference between these two methods,
i.e., mercury porosimetry measures all pores including dead-ended pores, whereas gas-liquid displacement only measures open pores.
Unsurprisingly, pure water flux of the Al
2O
3-YSZ seven-channel membrane declines with increasing sintering temperature (
Figure 7). The water flux dropped from 1642 to 586 LMH/bar when the sintering temperature was increased from 1400 to 1450 °C. The pure water flux is very sensitive to the sintering temperature at a range between 1430–1450 °C, which was 997 LMH/bar when sintered at 1430 °C and 904 LMH/bar when sintered at 1440 °C. They were considerably higher than the value of the 1450 °C sample, while the fracture load didn’t show significant changes. As a comparison, pure alumina seven-channel tubes showed much lower permeation rates, which was only 429 LMH/bar when sintered at 1400 °C and 120 LMH/bar when sintered at 1450 °C [
8]. Therefore, for the Al
2O
3-YSZ membranes, the best sintering temperature is 1430–1440 °C, at which both excellent mechanical property and good permeation characteristics can be obtained.
Figure 6.
Mercury intrusion porosimetry result of the Al2O3-YSZ membrane sintered at 1440 °C.
Figure 6.
Mercury intrusion porosimetry result of the Al2O3-YSZ membrane sintered at 1440 °C.
Figure 7.
Pure water fluxes of the Al
2O
3-YSZ membranes. Water fluxes of a pure alumina membrane with same structure [
8] are shown for comparison.
Figure 7.
Pure water fluxes of the Al
2O
3-YSZ membranes. Water fluxes of a pure alumina membrane with same structure [
8] are shown for comparison.