首页> 外文期刊>Journal of pharmaceutical sciences. >Rapid determination of vial heat transfer parameters using tunable diode laser absorption spectroscopy (TDLAS) in response to step-changes in pressure set-point during freeze-drying.
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Rapid determination of vial heat transfer parameters using tunable diode laser absorption spectroscopy (TDLAS) in response to step-changes in pressure set-point during freeze-drying.

机译:响应于冷冻干燥过程中压力设定值的阶跃变化,使用可调二极管激光吸收光谱法(TDLAS)快速确定样品瓶的传热参数。

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摘要

The purpose of this study was to perform a rapid determination of vial heat transfer parameters, that is, the contact parameter K(cs) and the separation distance l(v), using the sublimation rate profiles measured by tunable diode laser absorption spectroscopy (TDLAS). In this study, each size of vial was filled with pure water followed by a freeze-drying cycle using a LyoStar II dryer (FTS Systems) with step-changes of the chamber pressure set-point at to 25, 50, 100, 200, 300, and 400 mTorr. K(cs) was independently determined by nonlinear parameter estimation using the sublimation rates measured at the pressure set-point of 25 mTorr. After obtaining K(cs), the l(v) value for each vial size was determined by nonlinear parameter estimation using the pooled sublimation rate profiles obtained at 25 to 400 mTorr. The vial heat transfer coefficient K(v), as a function of the chamber pressure, was readily calculated, using the obtained K(cs) and l(v) values. It is interesting to note the significant difference in K(v) of two similar types of 10 mL Schott tubing vials, primary due to the geometry of the vial-bottom, as demonstrated by the images of the contact areas of the vial-bottom.
机译:这项研究的目的是使用可调谐二极管激光吸收光谱法(TDLAS)测量的升华率曲线,快速确定样品瓶的传热参数,即接触参数K(cs)和分离距离l(v)。 )。在这项研究中,每种规格的小瓶都装满纯净水,然后使用LyoStar II干燥机(FTS Systems)进行冷冻干燥循环,并将腔室压力设定值逐步更改为25、50、100、200, 300和400 mTorr。通过使用在25 mTorr的压力设定点测得的升华率,通过非线性参数估计独立确定K(cs)。在获得K(cs)之后,使用在25至400 mTorr下获得的合并升华速率分布图,通过非线性参数估计来确定每个样品瓶尺寸的l(v)值。使用获得的K(cs)和l(v)值,可以轻松计算出作为腔室压力的函数的样品瓶传热系数K(v)。有趣的是,注意到两种相似类型的10 mL肖特管样品瓶的K(v)存在显着差异,这主要是由于样品瓶底部的几何形状所致,如样品瓶底部接触区域的图像所示。

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