Shrinkage for the Z-axis leveled of

Shrinkage for the Z-axis leveled off at 39.68 percent and
39.69 percent, for firing temperatures of 746 and 7608C,
respectively, slow-axis shrinkage decreased from 30.48 percent
to 28.08 percent at 746 and 7608C, respectively, showing a
small expansion. This expansion was likely due to the
slumping effect that occurs when glass reaches a threshold
temperature known as the glass transition temperature TGand
begins to flow (Scholes, 1951; Zarzycki, 1991). Glass
transition temperatures are typically within the range of 530
to 1,3308C, depending on the type of glass (Le Bourhis,
2008). fast-axis shrinkage increased from 15.79 percent to
16.59 percent at 746 and 7608C, respectively, showing a trend
towards asymptotic behavior. In addition, Z-axis shrinkage
was by far the most profound, exhibiting 6-11 percent and
15-23 percent more shrinkage over the range of firing
temperatures than the slow- and fast-Axes, respectively. The
average shrinkage ratios for the slow- and fast-axis to the
Z-axis were 1:1.37 and 1:2.74, respectively. These extreme
differences can be attributed to the layer-by-layer production
method, binder burn-off, and inconsistencies in the recycled
glass stock.

結果 (中文) 1:

Z 轴收缩率趋于 39.68%和为 39.69%，烧成温度下的 746 和 7608 C，分别，慢轴收缩从 30.48%下降在 746 和 7608 C 28.08%，分别展示小的扩展。这种扩张是可能由于当玻璃达到阈值时发生的下滑影响温度称为玻璃化转变温度 TGand开始流 (斯科尔斯，1951 年;Zarzycki，1991年)。玻璃转型期的温度通常是 530 的范围内到 1，3308 C，玻璃 (Le Bourhis，类型2008 年).快速轴收缩增至 15.79%至16.59 %746 和 7608 C，分别呈现出的趋势对渐近行为。另外，z 轴收缩是到目前为止最为深刻的展出 6-11%和15-23%的烧成范围内更多收缩温度比慢和快-轴，分别。的平均收缩率为慢和快-轴向Z 轴分别为 1:1.37 和 1:2.74。这些极端差异可以归因于层由层生产方法、 粘合剂燃尽，和不一致之处的回收玻璃股票。

結果 (中文) 3:

对Z轴的收缩率稳定在百分之39.68，百分之39.69，为746和7608c烧成温度，分别是慢轴收缩率从百分之30.48百分之28.08在746和7608c，分别显示小膨胀。这种扩张很可能是由于下滑的影响，玻璃达到一个阈值时发生温度称为玻璃化转变温度、开始流动（斯科尔斯，1951；扎兹基，1991）。玻璃转变温度通常在530对13308c，取决于玻璃的类型（乐伯西斯，2008）。快速轴收缩率从百分之15.79提高到百分之16.59在746和7608c，分别呈现出的趋势渐近行为。此外，Z轴收缩是迄今为止最深刻，表现出6-11分15-23 %以上在射击范围收缩温度比慢速和快速轴，分别。这个慢和快速轴的平均收缩率Z轴分别为1.37和为2.74，分别。这些极端差异可以归因于层的层生产方法，粘合剂燃烧掉，和不一致的回收玻璃库存。