Study of Thermodynamic Properties of Nanomaterials for Different Size and Shape

2015 ◽  
Vol 17 (27) ◽  
pp. 17973-17979 ◽  
Author(s):  
H. Li ◽  
H. J. Xiao ◽  
T. S. Zhu ◽  
H. C. Xuan ◽  
M. Li

The size- and shape-related Ba/Bt functions.


2013 ◽  
Vol 2013 ◽  
pp. 1-5 ◽  
Author(s):  
R. Kumar ◽  
G. Sharma ◽  
M. Kumar

A simple theoretical model is developed to study the size and shape dependence of vibrational and thermodynamic properties of nanomaterials. To show the real connection with the nanomaterials we have studied Debye temperature, Debye frequency, melting entropy, and enthalpy in different shapes, namely, spherical, nanowire, and nanofilm of -Fe, Sn, Ag, and In. The results obtained are compared with the experimental data. A good agreement between the model predictions and the experimental data supports the theory developed in the present paper.


1988 ◽  
Vol 41 (1-2) ◽  
pp. 109-125 ◽  
Author(s):  
Edmundo Gomes de Azevedo ◽  
John M. Prausnitz

2017 ◽  
Vol 19 (13) ◽  
pp. 9016-9027 ◽  
Author(s):  
Bjørn A. Strøm ◽  
Jean-Marc Simon ◽  
Sondre K. Schnell ◽  
Signe Kjelstrup ◽  
Jianying He ◽  
...  

Size and shape effects on the thermodynamic properties of nanoscale volumes of water in molecular dynamics simulations, based on the nanothermodynamic formalism of Terrell L. Hill.


2017 ◽  
Vol 202 ◽  
pp. 177-183 ◽  
Author(s):  
Qingshan Fu ◽  
Zixiang Cui ◽  
Yongqiang Xue ◽  
Jinhua Zhu ◽  
Shaohui Guo

2018 ◽  
Vol 122 (27) ◽  
pp. 15713-15722 ◽  
Author(s):  
Qingshan Fu ◽  
Zixiang Cui ◽  
Yongqiang Xue ◽  
Huijuan Duan

1979 ◽  
Vol 44 ◽  
pp. 349-355
Author(s):  
R.W. Milkey

The focus of discussion in Working Group 3 was on the Thermodynamic Properties as determined spectroscopically, including the observational techniques and the theoretical modeling of physical processes responsible for the emission spectrum. Recent advances in observational techniques and theoretical concepts make this discussion particularly timely. It is wise to remember that the determination of thermodynamic parameters is not an end in itself and that these are interesting chiefly for what they can tell us about the energetics and mass transport in prominences.


Author(s):  
H.J.G. Gundersen

Previously, all stereological estimation of particle number and sizes were based on models and notoriously gave biased results, were very inefficient to use and difficult to justify. For all references to old methods and a direct comparison with unbiased methods see recent reviews.The publication in 1984 of the DISECTOR, the first unbiased stereological probe for sampling and counting 3—D objects irrespective of their size and shape, signalled the new era in stereology — and give rise to a number of remarkably simple and efficient techniques based on its distinct property: It is the only known way to obtain an unbiased sample of 3-D objects (cells, organelles, etc). The principle is simple: within a 2-D unbiased frame count or sample only cells which are not hit by a parallel plane at a known, small distance h.The area of the frame and h must be known, which might sometimes in itself be a problem, albeit usually a small one. A more severe problem may arise because these constants are known at the scale of the fixed, embedded and sectioned tissue which is often shrunken considerably.


Author(s):  
C J R Sheppard

The confocal microscope is now widely used in both biomedical and industrial applications for imaging, in three dimensions, objects with appreciable depth. There are now a range of different microscopes on the market, which have adopted a variety of different designs. The aim of this paper is to explore the effects on imaging performance of design parameters including the method of scanning, the type of detector, and the size and shape of the confocal aperture.It is becoming apparent that there is no such thing as an ideal confocal microscope: all systems have limitations and the best compromise depends on what the microscope is used for and how it is used. The most important compromise at present is between image quality and speed of scanning, which is particularly apparent when imaging with very weak signals. If great speed is not of importance, then the fundamental limitation for fluorescence imaging is the detection of sufficient numbers of photons before the fluorochrome bleaches.


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