A Dynamic Poisson's Ratio Measurement Method for Brittle Materials
A technology of brittle materials and measurement methods, which is applied in the direction of testing the strength of materials, measuring devices, and analyzing materials using one-time impact force. It can solve problems such as high cost, damage, and rapid rock failure process, and achieve accurate, reliable and adaptable results. , enhance the effect of authenticity and reliability
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Embodiment 1
[0083]The sample is a cuboid sample of blue sandstone, the size is: h×w×d=60mm×60mm×25mm; the angle α between the lenses of two high-speed cameras is 15°, and the lens with a focal length of 90mm is used, and the end surface of the lens is distanced from the sample for observation The distance to the surface is about 2000mm, the shooting resolution is set to 128×256pixels, and the shooting speed is 150,000 frames per second.
[0084] The method for measuring the dynamic Poisson's ratio of blue sandstone in this embodiment comprises the following steps: first, the blue sandstone rock sample is processed into a cuboid sample whose size is h×w×d=60mm×60mm×25mm, and then the sample is observed on the surface of the sample. To create an artificial speckle field, first clean the observation surface of the sample and then evenly spray white paint on it, and then use a special speckle stamp to make black speckle spots after it dries, such as Figure 4 shown; then according to the oper...
Embodiment 2
[0098] The sample is a marble cuboid sample, the sample size and test implementation steps are the same as in Example 1, and the loading rate is 1865GPa / s. The angle α between the lenses of the two high-speed cameras is 18°. A 100mm focal length lens is used. The distance between the lens end face and the sample observation surface is about 1200mm. The shooting resolution is set to 256×256pixels, and the shooting speed is 79161 frames per second. The measured elastic segment time (μs) on the dynamic stress-strain curve of the sample is (69, 109), and thus the digital image range (sheets) of the elastic segment is (5, 8); the starting and ending states of the elastic segment The full-field X-direction mean strain e under x-a =1.197×10 -3 、e x-b =5.638×10 -3 ; The average strain e in the Y direction y-a =-2.881×10 -5 、e y-b =-1.385×10 -3 ; Substituting the data, the sample dynamic Poisson's ratio μ=|e y-b -e y-a | / |e x-b -e x-a |=0.305.
Embodiment 3
[0100] The sample is a granite cylinder sample with a diameter of D = 50mm and a height of h = 50mm. The sample is placed between the SHPB horizontal impact devices by means of axial loading. The loading rate is 1747GPa / s. The test system is set and Implementation steps are the same as in Example 1. The measured elastic segment time (μs) on the dynamic stress-strain curve of the sample is (61, 112), and thus the digital image range (sheets) of the elastic segment is (9, 17); the starting and ending states of the elastic segment The full-field X-direction mean strain e under x-a =2.328×10 -3 、e x-b =4.875×10 -3 ; The average strain e in the Y direction y-a =-1.424×10 -4 、e y-b =-7.753×10 -4 ; Substituting the data, the sample dynamic Poisson's ratio μ=|e y-b -e y-a | / |e x-b -e x-a |=0.248.
[0101] As can be seen from the above description, the advantages of the dynamic Poisson's ratio measurement system and method for brittle materials of the present invention are:...
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