Atomic force microscopy (AFM), transmission electron microscopy (TEM) and scanning electron microscopy (SEM) of nanoscale plate-shaped second phase particles

被引:5
|
作者
Sobchenko, I.
Pesicka, J.
Baither, D.
Stracke, W.
Pretorius, T.
Chi, L.
Reichelt, R.
Nembach, E.
机构
[1] Univ Munster, Inst Mat Phys, D-48149 Munster, Germany
[2] Univ Munster, Univ Klinikum, Inst Med Phys & Biophys, D-48149 Munster, Germany
[3] Univ Munster, Inst Phys, D-48149 Munster, Germany
[4] Cherkasy Natl Univ, Dept Theoret Phys, UA-18031 Cherkassy, Ukraine
[5] Charles Univ Prague, Fac Math & Phys, Dept Met Phys, Prague 12116, Czech Republic
[6] Bremner Inst Angew Strahltech, D-28359 Bremen, Germany
关键词
D O I
10.1080/14786430701203184
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The feasibility of accurately measuring the size and the volume fraction of nanoscale plate-shaped precipitates by atomic force microscopy (AFM) has been explored. For quantitative evaluations their unhandy geometry is conveniently described by superellipsoids. The experimental alloy Ni69Co9Al18Ti4 served as a model system: plate-shaped disordered gamma-precipitates form in the L1(2) long-range ordered gamma'-matrix. The results obtained by AFM are compared with those derived from transmission (TEM) and from high-resolution scanning electron microscopy (SEM). The agreement between the AFM and the TEM results is good. In spite of the low number of SEM images taken, the same holds for the SEM results. In addition, magnetic force microscopy was applied; its results are acceptable. The main advantages of AFM are (i) the numerical output for all three dimensions, (ii) the simplicity of its operation and (iii) the lower cost of the microscope itself. The first point allows the numerical AFM output data to be directly subjected to automated computer-based evaluations. All present experimental and evaluation procedures are also applicable to cube-shaped particles with rounded edges and corners as found, for example, in gamma'-strengthened nickel-based superalloys.
引用
收藏
页码:2427 / 2460
页数:34
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