Dynamic property tests of frozen red sandstone using a split hopkinson pressure bar
In this study, frozen red sandstone specimens were impacted by a Split Hopkinson bar (SHPB), with a velocity of 4.558 ∼ 6.823 ms −1 . The temperature of the specimens was maintained at −15 °C during the experiment. For comparison purposes, static uniaxial compression tests were conducted in advance...
Saved in:
Published in | Earthquake Engineering and Engineering Vibration Vol. 18; no. 3; pp. 511 - 519 |
---|---|
Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
Harbin
Institute of Engineering Mechanics, China Earthquake Administration
01.07.2019
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
ISSN | 1671-3664 1993-503X |
DOI | 10.1007/s11803-019-0518-5 |
Cover
Summary: | In this study, frozen red sandstone specimens were impacted by a Split Hopkinson bar (SHPB), with a velocity of 4.558 ∼ 6.823 ms
−1
. The temperature of the specimens was maintained at −15 °C during the experiment. For comparison purposes, static uniaxial compression tests were conducted in advance using a freezing triaxial test machine. Four stress-strain curves were obtained in different average strain rates. The test results suggested that when the average strain rate is low, the specimen strength changes gradually; but when it is high, its strength changes rapidly. When the average strain rate is 120.73 s
−1
, the peak value of stress is as high as 82.96 MPa, which is about two times that of the static compressive strength of 44.1 MPa. A constitutive model was established that was composed of the damaged, viscoelastic and spring bodies, and revealed the variations of compressive strength and strain for the frozen red sandstone under different high strain rates. The test results also showed that the failure form was correlated to the average strain rate of the frozen red sandstone. When the average strain rate is low, the damage was only distributed on the specimen’s edges. However, as the average strain rate increases, the damage range extended to the central parts of the specimen. When the average strain rate reached 107.34s
−1
, the specimen was smashed. |
---|---|
Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
ISSN: | 1671-3664 1993-503X |
DOI: | 10.1007/s11803-019-0518-5 |