Lever question when lever is angled

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The discussion centers on the mechanics of a lever system configured at an angle, specifically analyzing the forces acting on a see-saw. The user presents a scenario where a 2kg force at 1m on one side and a 1kg force adjusted by the cosine of the angle at 2m on the other side are compared. The conclusion drawn is that the system will not achieve static equilibrium, as the left side's moment (2*1) exceeds the right side's moment (0.64*2). Additionally, the user questions the definition of distance in this context and notes that a point of support is necessary to maintain equilibrium.

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Hello, I have a question about a see-saw / lever problem. Does this configuration I have shown here allow me to treat the system like a regular lever if I make the downward force at the horizontal point from the center to be the cosine of the angle? In this example the downward force on the left would be 2kg at 1m whereas on the right it would be 1kg * cos(5) at 2m.

Based on the static equilibrium equation of a lever F1*d1= F2*d2 the system would not be in equilibrium and would fall to the left. 2*1 > 0.64*2

Is this correct?

Would that mean that there is a compression force of the sine of the angle down the shaft towards the fulcrum on the right side? 1kg*sin(50) ?
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In this example the downward force on the left would be 2kg at 1m whereas on the right it would be 1kg * cos(5) at 2m.

How do you define the distance?

Based on the static equilibrium equation of a lever F1*d1= F2*d2 the system would not be in equilibrium and would fall to the left. 2*1 > 0.64*2p

The object will fall unless a 1m point is made to hold. If this is done, then it'll be a net equilibrium.

No it will not rotate while falling due to gravity.
 

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