principal stress sentence in Hindi
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- In the case of normal faults, the rock mass is pushed down in a vertical direction, thus the pushing force ( "'greatest "'principal stress ) equals the weight of the rock mass itself.
- In the case of thrusting, the rock mass'escapes'in the direction of the least principal stress, namely upward, lifting the rock mass up, thus the overburden equals the "'least "'principal stress.
- In the case of thrusting, the rock mass'escapes'in the direction of the least principal stress, namely upward, lifting the rock mass up, thus the overburden equals the "'least "'principal stress.
- Using the double angle approach we measure the angles " BOC and " BOE in the Mohr Circle ( Figure 8 ) to find double the angle the major principal stress and the minor principal stress make with plane B in the physical space.
- Using the double angle approach we measure the angles " BOC and " BOE in the Mohr Circle ( Figure 8 ) to find double the angle the major principal stress and the minor principal stress make with plane B in the physical space.
- As the faces slide in opposite directions, tension is created at the tip, and a mode I fracture is created in the direction of the " ? h-max ", which is the direction of maximum principal stress.
- It is assumed that the brittle material has no tensile strength . ( In case of reinforced concrete this assumption is necessary because the concrete has small shrinkage cracks . ) Therefore, the principal stresses of the brittle material need to be compression.
- To determine the equation of the stress ellipsoid we consider the coordinate axes x _ 1, x _ 2, x _ 3 \, \ ! taken in the directions of the principal axes, i . e ., in a principal stress space.
- Secondly, a \ D * a works, were a is a standard rotation matrix about an axis, i . e . for the 1-3 plane ( if sigma1 was the highest principal stress and sigma3 was the lowest ), it would be:
- Other examples of sets of tensor invariants are the set of principal stresses ( \ sigma _ 1, \ sigma _ 2, \ sigma _ 3 ) or the set of mechanics invariants ( I _ 1, J _ 2, J _ 3 ).
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