Force parallel to a smooth wall?

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A smooth wall exerts a force that is strictly perpendicular to it, as the term "smooth" implies the absence of friction. In the context of a see-saw positioned against such a wall, the wall's reaction force is responsible for balancing the moments created by the see-saw's weight. While hinges can exert forces in multiple directions, a frictionless hinge must still provide some form of resistance to prevent the attached object from falling. The reaction force at the pivot of the see-saw is also perpendicular to the see-saw itself, ensuring that all forces and torques are balanced. Overall, the dynamics of the system depend on the geometry and positioning of the see-saw and pivot.
21joanna12
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Hello!

My question is quite a quick one- I was wondering whether it is ever possible to have a smooth wall exerting a force parallel to it (and not just perpendicular to it). For example, if you were to place a see-saw by a smooth wall so that the wall is holding one of the see-saw ends below the level of the other, is this only due to the moment because of the perpendicular, reaction force from the wall or is there also a force parallel to the wall exerted by it (in the line that friction would act). I seem to remember seeing a question like this before, although I cannot remember whether the force perpendicular to the smooth wall was only in the case of an object being attached (for example by a hinge) to the wall, or if it also applies to objects 'propped up', but not attached to, the wall as in the see-saw case.

Also, when considering the see-saw and assuming that the pivot of the see saw is propped up on a knife edge to create the pivot, would the reaction force from this pivot act vertically upwards, or would it be perpendicular to the line of the see-saw?

I apologise if I haven't explained this very clearly...

Thank you in advance!

EDIT: I think I figured out my second question about whether the force from the pivot is vertical or perpendicular to the see-saw plank. I think It must be perpendicular, because otherwise there the weight of the see saw, and the reaction force (and potentially the force at the wall which is parallel to the wall, whether it is friction or another force) would all be acting vertically and there would be no force to cancel the horizontal normal contact force at the wall... I think...
 
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21joanna12 said:
Hello!

My question is quite a quick one- I was wondering whether it is ever possible to have a smooth wall exerting a force parallel to it (and not just perpendicular to it). For example, if you were to place a see-saw by a smooth wall so that the wall is holding one of the see-saw ends below the level of the other, is this only due to the moment because of the perpendicular, reaction force from the wall or is there also a force parallel to the wall exerted by it (in the line that friction would act).

The expression "smooth wall" usually means there is no friction - so the reaction force must be perpendicular.
 
CWatters said:
The expression "smooth wall" usually means there is no friction - so the reaction force must be perpendicular.

Thank you for your reply! But can there really be no other force? I'm pretty sure that dealing with hinges, there was a force parallel to the wall despite the fact that the hing was smooth. Could the same principle not apply?
 
21joanna12 said:
Thank you for your reply! But can there really be no other force? I'm pretty sure that dealing with hinges, there was a force parallel to the wall despite the fact that the hing was smooth. Could the same principle not apply?

A hinge can be frictionless in rotation but must provide friction in other directions (parallel and perpendicular to the wall) or the door would fall off.
 
Perhaps this diagram helps.
smooth wall.png


The triangular pivot is fixed in space. The purple reaction force need not be perpendicular to the seesaw. Nothing is accelerating so all forces and torques sum to zero.

The "red" force must be perpendicular to the smooth/frictionless wall. The magnitude of the red force depends on the geometry and can be calculated because the torques must sum to zero (The 10kg/100N blue force creates an anticlockwise torque that must be countered by the red force).

Perhaps consider what happens if you reposition the seesaw so that it is almost horizontal. The magnitude of the red force would have to be very large, as would the red component of the reaction force at the pivot. If the pivot was just a knife blade it's possible there wouldn't be enough friction at the pivot.
 
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Thank you both!
 
I do not have a good working knowledge of physics yet. I tried to piece this together but after researching this, I couldn’t figure out the correct laws of physics to combine to develop a formula to answer this question. Ex. 1 - A moving object impacts a static object at a constant velocity. Ex. 2 - A moving object impacts a static object at the same velocity but is accelerating at the moment of impact. Assuming the mass of the objects is the same and the velocity at the moment of impact...

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