Normal Force on Extended Block: Physics Explained

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SUMMARY

The discussion centers on the behavior of normal force acting on an extended block resting on a frictionless surface. It is established that the normal force can act at various points depending on the block's shape and surface contact, including as a distributed force, at a point, along a line, or at multiple points. In simple scenarios, such as a block sliding down a slope, the normal force is typically modeled as acting through the center of mass. For more complex situations, like a box tipping over, the normal force may be represented as acting along an edge, particularly just after tipping begins.

PREREQUISITES
  • Understanding of normal force in physics
  • Familiarity with frictionless surfaces
  • Knowledge of distributed forces versus point forces
  • Basic principles of static equilibrium
NEXT STEPS
  • Study the concept of distributed forces in physics
  • Learn about the coefficient of friction and its experimental determination
  • Explore the dynamics of tipping objects and the role of normal force
  • Investigate the effects of surface irregularities on force distribution
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Physics students, educators, and anyone interested in understanding the mechanics of forces acting on objects in various scenarios, particularly in relation to normal force and frictionless surfaces.

Jon Drake
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Suppose there is an extended block lying on a frictionless surface. The surface will exert a normal force on block. Will the normal force act at one particular point on the block, or will it act along the entire length of block?
 
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The Normal Force is a simplified model of how the block and surface interact. In practice it depends how flat the block and surfaces are. A warped piece of wood might only make contact at say three corners. A very soft rubber block would make a more uniform contact.

Depending on the exact set up and what you are trying to calculate you might need to model and/or position the normal force differently, for example as either:

a distributed force or
acting at a point
acting on a line
acting at a number of individual points.

For most simple problems such as block sliding down a slope we assume a single force acting through the centre of mass. Any complication due to the block or surface not being exactly flat is hidden in the coefficient of friction (which is typically found by experiment rather than calculated).

For something like a box being tipped over we might model the normal force as acting along one edge (which would be the case just after it starts to tip).

If you have a particular problem in mind perhaps post details.
 
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PS You mention the frictionless case. The key thing to understand with frictionless surfaces is that any force between them must be perpendicular/normal to the surface.
 

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