geomane
Geotechnical
- Apr 4, 2013
- 199
For the rankine active earth pressure case, the wall moves a sufficient distance away from the soil mass causing the soil to fail on a plane of 45 + phi/2 with the horizontal. This is true for a granular soil with no cohesion. If you completely removed the wall away from the soil, the soil should stabilize at the phi angle (stable slope angle = phi angle).
We had a question come up in the office today of why wouldn't the active earth pressure failure plane equal the phi angle, when the wall only slightly moved away from the soil mass (enough movement for the active case). The way I look at it is, if the the wall is moved only enough to cause the soil to fail, you still have confining pressure, which keeps your mohr circle to the right (higher stresses) than zero. So at the point where the mohr circle touches the mohr-circle failure envelope, that point is at angle of 45 + phi/2 measured from the horizontal.
I'm having trouble explaining the case with the wall completely removed in terms of mohrs circles and failure plains, other than when you remove the wall completely, you remove the confining pressures.
Can someone please provide a better explanation on this?
We had a question come up in the office today of why wouldn't the active earth pressure failure plane equal the phi angle, when the wall only slightly moved away from the soil mass (enough movement for the active case). The way I look at it is, if the the wall is moved only enough to cause the soil to fail, you still have confining pressure, which keeps your mohr circle to the right (higher stresses) than zero. So at the point where the mohr circle touches the mohr-circle failure envelope, that point is at angle of 45 + phi/2 measured from the horizontal.
I'm having trouble explaining the case with the wall completely removed in terms of mohrs circles and failure plains, other than when you remove the wall completely, you remove the confining pressures.
Can someone please provide a better explanation on this?