another thought
...
But FORCE, that is another matter. In a conventional (flat) backcut the forces generated as the wedge goes in are ONE a bigger one trying to move the two sides of the backcut apart. this is the useful effect we are movign the tip of the tree with to get it to go over in the desired direction.
--- and TWO a lesser force from friction trying to push the stump over forwards, and by pushing the bottom of the bole forwrds cause rotation of the tree backwards. BUT neither of these things happen in a typcial cut, as the stump to be is too firmly rooted to rotate under the axe or hammer blows. And if the base dont move, and the hinge dont fail the only movement of the bole will be to roatate as the wedging TORQUE is trying to do.
Back to force ONE above, if you diagram it out you will see the force from the wedge that is trying to open the sloped backcut has a large component pusing forwards on the bole of the tree trying to shear the hinge and move the bole off the stump. Possibly before the tree has committed to going the pro0per direction~!
TD, in trying to extend what you have so clearly presented, I began to realize how complicated this whole thing gets when you leave the simple world of classical physics and start thinking about all the possible ways real wood is going to screw up the simple equations.
You rightly mention the friction between the wedge and the two faces of the kerf. We should add to your enumeration of the assumptions of the classical anaysis the assumption of a frictionless wedge. The frictional force on a real wedge is actually going to be enormous given the tremendous weight of the tree normal to the wedge, and we are certainly going to have to account for it in a more complete analysis.
In the ideal case of a frictionless wedge, the only forces between the tree and the wedge will act perpendicular to the wedge faces.
--- and TWO a lesser force from friction trying to push the stump over forwards, and by pushing the bottom of the bole forwrds cause rotation of the tree backwards. BUT neither of these things happen in a typcial cut, as the stump to be is too firmly rooted to rotate under the axe or hammer blows. And if the base dont move, and the hinge dont fail the only movement of the bole will be to roatate as the wedging TORQUE is trying to do.
The frictional forces of the real wedge act parallel to the wedge faces. For the upper face in the flat backcut the friction, as you drive in the wedge, acts to push the bole forward (as you noted). Isn't this just the "shear" force that everyone is so worried about that tends to break the hinge? Now it may be larger in a slanted backcut, but it seems it will be present in a flat backcut as well.
There seems to be universal agreement here that wedging a slanted backcut is much more likely to break the hinge, and maybe this is true, but I think someone needs to show that it is.
Here is a contrary thought that shows why I retain a bit of skepticism about this claim. Forget the wedge for a moment, but hang on to the hammer. Swing hard and hit the bole right above the backcut, trying to drive the bole off the stump. Now go up 30 feet and do the same swing striking directly above the first contact. The force vector is identical in both cases--the dreaded horizontal "shear" force that wants to break the hinge. But does anyone believe those two hammer blows are equally likely to be successful? It seems that distance from the hinge is a factor we must consider.
This is an excellent problem, and there is certainly much more to it than has been discussed so far. I look forward to hearing what others have to say.