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A microscopic model of the Tian-Calvet microcalorimeter, cell design for a faster response, and measurement by a continuous procedure

机译:Tian-Calvet微量热量计的微观模型,快速响应的细胞设计以及通过连续程序进行测量

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The transient heat conduction equation was used as the microscopic model of the Tian-Calvet microcalorimeter. It was verified by comparing simulated and experimental calorimetric curves and used to guide sample cell design for a faster response time, for which it gave the guidelines to minimize the heat flow distance and use a heat flux that is uniform and onto the whole face of the thermopile sensor. The resulting sample cell was disc-shaped with the sample powder placed in it as a thin 0.2 mm layer on a stainless steel base with a wall thickness of 0.5 mm that covered the whole face of the thermopile on which it was placed. The rise time of the heat response curve to a step change in sample temperature, which is the response time for measuring the differential heat released, was 45 s. The response curve from a gas dose returned to the baseline within 400 s, which is the time needed to measure the integrated heat in a pulsed dosage. The accuracy of the heats measured by the calorimeter was verified by comparison with data in the literature on the adsorption of ethanol and ammonia on HZSM-5 and adsorption of methanol and ammonia on SAPO-34. The differential heat of methanol adsorption on SAPO-34 at 333 K and ammonia adsorption on HZSM-5 at 423 K were measured by both the conventional discontinuous procedure and a new continuous procedure. In the continuous procedure, gas was continuously dosed at a very slow flow rate that was kept slow enough for the gas and adsorbate to reach quasi-equilibrium. The continuous procedure has the advantages of high resolution results and a simpler experimental procedure, and a calorimetric curve could be measured within 3 h.
机译:瞬态热传导方程用作Tian-Calvet微热量计的微观模型。通过比较模拟量热曲线和实验量热曲线进行了验证,并将其用于指导样品池设计以加快响应时间,为此,它提供了最小化热流距离并使用均匀且遍布整个表面的热通量的准则。热电堆传感器。所得的样品池为圆盘形,样品粉以0.2毫米的薄层放置在不锈钢底座上,壁厚为0.5毫米,覆盖了其所放置的热电堆的整个表面,壁厚为0.5毫米。热响应曲线对样品温度的阶跃变化的上升时间为45 s,这是用于测量释放的差热的响应时间。气体剂量的响应曲线在400 s内返回基线,这是测量脉冲剂量下的积分热量所需的时间。通过量热仪测量的热量的准确性通过与文献中有关乙醇和氨在HZSM-5上的吸附以及甲醇和氨在SAPO-34上的吸附的文献进行比较来验证。通过常规的不连续程序和新的连续程序,分别测量了在333 K时SAPO-34上甲醇吸附和423 K在HZSM-5上氨吸附的差热。在连续过程中,以非常缓慢的流速连续计量气体,该流速应保持足够缓慢,以使气体和被吸附物达到准平衡。连续程序具有高分辨率的结果和简单的实验程序的优点,并且可以在3小时内测量量热曲线。

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