Modeling creep and creep recovery of 332 aluminum alloy using fractional calculus

Author(s):  
Wenping Fan ◽  
Yang Huang
2014 ◽  
Vol 49 (1-2) ◽  
pp. 45-55 ◽  
Author(s):  
Alberto Sapora ◽  
Pietro Cornetti ◽  
Alberto Carpinteri ◽  
Orazio Baglieri ◽  
Ezio Santagata

2021 ◽  
pp. 107183
Author(s):  
Thais C. Brito-Oliveira ◽  
Izabel C.F. Moraes ◽  
Samantha C. Pinho ◽  
Osvaldo H. Campanella

1984 ◽  
Vol 51 (4) ◽  
pp. 816-820 ◽  
Author(s):  
U. W. Cho ◽  
W. N. Findley

Creep and creep recovery data are reported for pure tension of 2618-T61 aluminum alloy under variable temperature between 200° C and 230° C. Varying temperature experiments involved an abrupt temperature increase and a linearly increasing and decreasing temperature at a constant stress of 137.9 MPa (20 ksi). A temperature-compensated time by Sherby and Dorn was employed to represent the effect of temperature. A temperature-history-dependent theory using data from constant stress creep and creep recovery together with the apparent activation energy was used to predict the creep under variable temperature. The predictions agreed quite well with the observed data. The apparent activation energy of this alloy was found to be 49,000 cal/mole°K.


Author(s):  
G. G. Shaw

The morphology and composition of the fiber-matrix interface can best be studied by transmission electron microscopy and electron diffraction. For some composites satisfactory samples can be prepared by electropolishing. For others such as aluminum alloy-boron composites ion erosion is necessary.When one wishes to examine a specimen with the electron beam perpendicular to the fiber, preparation is as follows: A 1/8 in. disk is cut from the sample with a cylindrical tool by spark machining. Thin slices, 5 mils thick, containing one row of fibers, are then, spark-machined from the disk. After spark machining, the slice is carefully polished with diamond paste until the row of fibers is exposed on each side, as shown in Figure 1.In the case where examination is desired with the electron beam parallel to the fiber, preparation is as follows: Experimental composites are usually 50 mils or less in thickness so an auxiliary holder is necessary during ion milling and for easy transfer to the electron microscope. This holder is pure aluminum sheet, 3 mils thick.


2015 ◽  
Vol 30 (6) ◽  
pp. 627
Author(s):  
YE Zuo-Yan ◽  
LIU Dao-Xin ◽  
LI Chong-Yang ◽  
ZHANG Xiao-Hua ◽  
ZANG Xiao-Ming ◽  
...  

Equipment ◽  
2006 ◽  
Author(s):  
S. R. Carvalho ◽  
S. M. M. Lima e Silva ◽  
G. Guimaraes

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