Problem dealing with Equilibrium & Torque

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A 40 kg beam supported by two posts is analyzed for stability as a 20 kg boy walks along it. The equilibrium conditions require that both the sum of torques and the sum of forces equal zero. The calculations reveal that the boy can walk up to 4 meters from the left end without tipping the beam. To find the force on the other support when the beam is about to tip, one must consider the pivot point and the weight distribution. Understanding the weight's point of action and the pivoting support is crucial for solving the problem accurately.
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Homework Statement



A 40 kg, 5.0-m-long beam is supported by, but not attached to, the two posts. A 20 kg boy starts walking along the beam. How close can he get to the right end of the beam without it tipping?

The left post under the very left end of the beam, and the first post is 3.0 m to the right of it. I've attached an image to assist in visualizing.

Homework Equations



To be in equilibrium:
\sum \vec{\tau} = 0
\sum \vec{F} = 0

Torque:
\vec{\tau} = r \cdot \vec{F_\perp}

Weight:
\vec{w} = m \cdot \vec{g}

The Attempt at a Solution



Since I know the Torque must be 0 to keep the beam from rotating, I get:

40 \cdot 9.8 + 20 \cdot 9.8 = 3 \cdot \vec{F}_\text{right beam}
3 is the distance from the pivot point (the left beam) to the right beam and F2 is force of the right post.

Fnet must also be 0, so I get the following:

\vec{F}_\text{left beam} + \vec{F}_\text{right beam} = 40 \cdot 9.8 + 20 \cdot 9.8

I'm stuck because I've got 2 functions and 3 unknown variables (Fleft beam, Fright beam, x (distance from the pivot point to the boy)).

I assume there is a way to find these but I'm not sure where to go from here or if I've made a mistake.
 

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Hints:
Where does the weight of the beam act?
When the beam is just about to tip, about which support is it pivoting? At that point, what's the force at the other support?
 
Thank you for the hints! Your 2nd hint is what led me to figure it out, your first hint made me realize that I messed up showing my work in Latex (sorry if that confused you).

Anyway, I got 4 m when solving for x, which looks right!
 
Excellent.
 
alprim said:
How do I figure out what the force on the other support is?
If the board is just about to tip, what must be the force on the other support?

(Realize that you are replying to a thread that is several years old.)
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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