The ladder tends to slip more when the man stands near the wall.
Let us first draw a diagram to understand the problem. AB is the ladder with end A resting on the ground and end B against the wall. OA = d, OB = h, and W is the weight of the man on the ladder at distance x from end A horizontally. R and R' are normal forces at the ends A and B also F and F' are friction forces at A and B.
![](https://www.sarthaks.com/?qa=blob&qa_blobid=13981478888830538862)
Assuming µ same at both contact surfaces,
F =µR, F' = µR'
Equating forces vertically,
R+F' =W
R+µR' =W
Equating forces horizontally
F = R'
Taking Moments of all forces about B, we have
W(d-x)+Fh-Rd = 0 →W(d-x)+µRh-Rd = 0
→W(d-x) = R(d-µh)
→R=W(d-x)/(d-µh)
Overturning Torque (anticlockwise) about A
= Wx
Restoring torque (Clockwise)
= R'h+F'd
So net overturning torque T
=Wx-(R'h+F'd)
=Wx-(Fh+µR'd)
=Wx-(Fh+µFd)
=Wx-F(h+µd)
=Wx-µR(h+µd)
=Wx-µW(d-x)(h+µd)/(d-µh)
={Wxd-Wxµh-µW(dh+µd²-xh-µxd)}/(d-µh)
={Wxd-Wxµh-µWdh+µ²d²W+µxhW+µ²Wxd)}/(d-µh)
={Wxd(1+µ²)+Wµd(µd-h)}/(d-µh)
In this expression all except x are constant and we can see that as x increases T also increases.
So, the ladder tends to slip more when the man stands near the wall.