Leo W. answered 05/21/24
PhD in Applied Math, BS in Physics and Math with minor in CS
Not giving a specific answer in case this is a graded problem.
However, the approach is pretty standard.
- Set up a free body diagram with a ladder leaning against a wall with angle θ from the floor. There are five forces acting at different points on the ladder
- FNx - the normal force of the wall acting horizontally away from the wall at the top of the ladder
- FW = Mg - the weight of the man on the ladder acting downward at some unknown distance d up the ladder
- Fw = mg - the weight of the ladder acting downward at a point a distance L/2 up the ladder (length L)
- FNy - the normal force of the floor acting vertically upward from the floor on the foot of the ladder
- Ff = μ FNy - the force of friction acting horizontally toward the wall on the foot of the ladder to keep it from sliding out
- Set up equations balancing the horizontal forces FNx and Ff, the vertical forces FW, Fw, and FNy and finally the torques about a somewhat arbitrary pivot at the foot of the ladder. These torques are FNxL sinθ clockwise, and FWdcosθ, and FwLcosθ/2.counterclockwise.
- Use substitution and algebra to solve for the unknown d in the last equation in terms of known values