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Hi all, this is a problem with which I led myself in circles with for hours, because I kept forgetting to factor in a different thing each time. Long story short, I thought I'd cracked it, but my answer and the given answer are out by a square. Please see my efforts below!
A uniform ladder of mass M and length L stands on rough horizontal ground and leans against a vertical wall with which it makes an angle θ. A man of mass m stands on the ladder a distance x from the bottom.
a) obtain expressions for the normal reaction and the friction force acting at the point of contact between the ladder and the ground.
The normal is obviously (m+M)g.
Other than that, it's static equilibrium, and the equation I used for balancing was the moments, where τNW is the moment due to the normal FNW to the wall at the top of the ladder, and τMg and τmg are the two moments of the ladder and man:
1. τNW = τMg + τmg
Pretty simple. I have the ladder to be length L, so I set the origin of turning at the base of the ladder. I want to find FNW because it's equal to the frictional force FF at the base of the ladder.
The radius component for the moment τNW is this Lcosθ. The moment is thus: FNWLcosθ.
The radius component for τMg is (L/2)sinθ, and for τmg is (x/L)sinθ.
So the two moments are: [(MgL)/2]sinθ and [(mgx)/L]sinθ
Equation 1. then becomes:
FNWLcosθ = [(MgL)/2]sinθ + [(mgx)/L]sinθ
Which evidently becomes, solving for FNW:
FNW = (M/2 + mx/L2)gtanθ
In the given answer, the mx/L2 term is simply mx/L. But the position of the man along the ladder was given as x from the bottom, so this should be written x/L, right? Which means dividing out the L on the FNW side will always create a squared term.
Any insight appreciated.
Jack
Homework Statement
A uniform ladder of mass M and length L stands on rough horizontal ground and leans against a vertical wall with which it makes an angle θ. A man of mass m stands on the ladder a distance x from the bottom.
a) obtain expressions for the normal reaction and the friction force acting at the point of contact between the ladder and the ground.
Homework Equations
The normal is obviously (m+M)g.
Other than that, it's static equilibrium, and the equation I used for balancing was the moments, where τNW is the moment due to the normal FNW to the wall at the top of the ladder, and τMg and τmg are the two moments of the ladder and man:
1. τNW = τMg + τmg
The Attempt at a Solution
Pretty simple. I have the ladder to be length L, so I set the origin of turning at the base of the ladder. I want to find FNW because it's equal to the frictional force FF at the base of the ladder.
The radius component for the moment τNW is this Lcosθ. The moment is thus: FNWLcosθ.
The radius component for τMg is (L/2)sinθ, and for τmg is (x/L)sinθ.
So the two moments are: [(MgL)/2]sinθ and [(mgx)/L]sinθ
Equation 1. then becomes:
FNWLcosθ = [(MgL)/2]sinθ + [(mgx)/L]sinθ
Which evidently becomes, solving for FNW:
FNW = (M/2 + mx/L2)gtanθ
In the given answer, the mx/L2 term is simply mx/L. But the position of the man along the ladder was given as x from the bottom, so this should be written x/L, right? Which means dividing out the L on the FNW side will always create a squared term.
Any insight appreciated.
Jack