RPstress
Aerospace
- Jun 4, 2003
- 846
We recently had a failure of a test specimen which we couldn't explain, except for a mechanism like that sketched in the engineering.com picture. (Hopefully that works; it's listed as an 'attachment' in the preview.)
Has anyone got any opinions about the viability of the idea? A quick check on Euler properties doesn't rule it out.
(If crack is 25 mm long and four-point specimen is 2 mm thick total and 10 mm wide and QI HS carbon it might have Euler_stress = 4.π2.50000.(13.10/12) / 252 / (1.10) = 260 MPa average, maybe 500 MPa peak...)
However, intuitively it seems unlikely. Maybe if the curvature was not too great (flatter than in my sketch)? It looks like it needs a delamination to start with. Could this possibly happen with no delam?
The extreme plies under maximum compression seem to pop off in a failure mode similar to Euler instability, presumably modified by an elastic foundation effect due to being part of the laminate. This seems to happen to the extreme ply if it's at 0° and gives a buckle length of about 10 mm with no obvious fibre failure. Plies are about 0.25 mm thick.
Has anyone got any opinions about the viability of the idea? A quick check on Euler properties doesn't rule it out.
(If crack is 25 mm long and four-point specimen is 2 mm thick total and 10 mm wide and QI HS carbon it might have Euler_stress = 4.π2.50000.(13.10/12) / 252 / (1.10) = 260 MPa average, maybe 500 MPa peak...)
However, intuitively it seems unlikely. Maybe if the curvature was not too great (flatter than in my sketch)? It looks like it needs a delamination to start with. Could this possibly happen with no delam?
The extreme plies under maximum compression seem to pop off in a failure mode similar to Euler instability, presumably modified by an elastic foundation effect due to being part of the laminate. This seems to happen to the extreme ply if it's at 0° and gives a buckle length of about 10 mm with no obvious fibre failure. Plies are about 0.25 mm thick.