Normal Force and Atmospheric Pressure

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Discussion Overview

The discussion revolves around the forces acting on a cube at rest on a horizontal surface, specifically focusing on the role of normal force, gravitational force, and atmospheric pressure. Participants explore the implications of atmospheric pressure on the normal force and the conditions under which these forces interact, touching on concepts of buoyancy and the effects of air pressure.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant asserts that the normal force N should equal the gravitational force plus the atmospheric pressure acting on the top face of the cube, questioning why N is often simplified to N = mg.
  • Another participant argues that atmospheric pressure actually acts to buoy objects upwards, suggesting that there is air underneath the cube unless it is sealed, which complicates the analysis.
  • A later reply emphasizes that the buoyancy effect of atmospheric pressure is small and that other factors, such as variations in gravitational acceleration and the Earth's rotation, should also be considered in calculating the normal force.
  • Some participants mention the concept of "wringability" in relation to gauge blocks, indicating that air pressure is not the only factor affecting their adhesion.

Areas of Agreement / Disagreement

Participants express differing views on the significance of atmospheric pressure and buoyancy in relation to the normal force. There is no consensus on how to incorporate these factors into the analysis of forces acting on the cube.

Contextual Notes

Participants highlight the complexity of the situation, noting that gravitational acceleration is not constant and that the effects of Earth's rotation must be accounted for. The discussion also raises questions about the presence of air between the cube and the surface, which remains unresolved.

Sukuya
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1. Suppose a cube of mass m is lying at rest on a horizontal surface. The area of one face of the cube is A. For the equlibrium of cube no net force acts on it. If we consider the vertical direction then the contact force N should be equal to the force due to gravity plus the force due to atmospheric pressure acting on the top face. There is no air between bottom face and the horizontal surface so atmospheric pressure is not acting on the bottom face. The atmospheric pressure is substantial too, so we can't ignore it. Still we say that N = mg instead of N = mg + PA, where P is the atmospheric pressure. Why ?
 
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If there were actually no air between the bottom of the object and the surface, then the air pressure would be significant. In fact, that is how suction cups work (there isn't "no air" under a suction cup, but the pressure is lowered when you pull upwards on the suction cup and increase the volume of the region between the cup and the table).

This should convince you that most real objects do not seal tightly enough against the table to exclude air.
 
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Perhaps worth a look at "Wringability" of gauge blocks. (edit...but it's not just air pressure that keeps them together).
 
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Sukuya said:
If we consider the vertical direction then the contact force N should be equal to the force due to gravity plus the force due to atmospheric pressure acting on the top face. There is no air between bottom face and the horizontal surface so atmospheric pressure is not acting on the bottom face. The atmospheric pressure is substantial too, so we can't ignore it. Still we say that N = mg instead of N = mg + PA, where P is the atmospheric pressure. Why ?

You have the sign wrong. Atmospheric pressure buoys objects upwards rather than pushing them down. There is air underneath your block unless you take extreme measures to seal the bottom of your cube.

So why don't we use this buoyancy-corrected weight? Simple: It's a tiny effect. You ignored a couple of other tiny effects when you said "N=mg". Gravitation acceleration is not constant everywhere. You should be using N=mg(x), where g(x) is the gravitational acceleration at the location of interest. Even that is not correct because the Earth is rotating at one revolution per sidereal day. The net force on your cube has to be just the amount needed to make the cube rotate at this rate at about the Earth's rotation axis.
 
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D H said:
You have the sign wrong. Atmospheric pressure buoys objects upwards rather than pushing them down. There is air underneath your block unless you take extreme measures to seal the bottom of your cube.

So why don't we use this buoyancy-corrected weight? Simple: It's a tiny effect. You ignored a couple of other tiny effects when you said "N=mg". Gravitation acceleration is not constant everywhere. You should be using N=mg(x), where g(x) is the gravitational acceleration at the location of interest. Even that is not correct because the Earth is rotating at one revolution per sidereal day. The net force on your cube has to be just the amount needed to make the cube rotate at this rate at about the Earth's rotation axis.

What I wasn't able to convince myself was that there was air between the block and the surface, which tantamounts to air only pushing it down. Of course the g we take is the effective g taking into consideration of Earth's rotational effects as well as variation with height/depths etc.
 
CWatters said:
Perhaps worth a look at "Wringability" of gauge blocks. (edit...but it's not just air pressure that keeps them together).

I looked up wringability just to see what they say.
and I got more sites on Writing Ability than wringability.
I encountered the blocks only once many eons ago.
 

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