Define Individual Forces Acting on a Body

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Discussion Overview

The discussion revolves around the definition and application of individual forces acting on a body, particularly in the context of Newton's laws of motion. Participants explore how to conceptualize and measure forces, especially in dynamic systems, and the relationship between force, mass, and acceleration.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants seek a clear definition of individual forces and how they can be applied to a body in motion.
  • One participant suggests tracing the source of a force applied to a body to understand its magnitude and direction.
  • Another participant notes the difficulty in explaining how constant forces are applied in dynamic systems, mentioning friction and spring forces as examples.
  • A participant argues that F = ma is not a definition of force but rather a relationship that defines mass, while also discussing the distinction between contact forces and body forces like gravity.
  • Some participants express confusion regarding the interpretation of F = ma as a definition of mass and the implications of Newton's laws.
  • One participant introduces the concept of impulse and its relation to force, suggesting that the original formulation of Newton's second law involves momentum rather than force directly.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the definition of individual forces or the interpretation of F = ma. Multiple competing views are presented regarding the nature of force and its relationship to mass and acceleration.

Contextual Notes

The discussion highlights various interpretations of fundamental concepts in physics, such as the definitions of force and mass, and the application of these concepts in different scenarios. There are unresolved questions regarding the application of forces in dynamic systems and the foundational principles of Newtonian mechanics.

Viru.universe
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0k i know net force on a body is defined as mass times acceleration of the body w.r.t inertial frame,
but how do we define individual forces acting on the body?
Eg. Forces acting on a 1kg block are F1=+6¡ And F2=-4¡
So we know net force=2¡, and net acceleration=2 m/s^2
but how do we actually apply something called "6 N" force in right direction, and "4 N" in left direction?
Thank you.
 
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Hi Viru.universe! :smile:
Viru.universe said:
Eg. Forces acting on a 1kg block are F1=+6¡ And F2=-4¡
So we know net force=2¡, and net acceleration=2 m/s^2
but how do we actually apply something called "6 N" force in right direction, and "4 N" in left direction?

We follow the trail!

If a force is applied to the body at a particular point, just trace it back to its source, and then the amount of the force will be obvious.

Eg, if a mass on a table is being pulled by two horizontal strings going over pulleys and joined to weights, then the individual force on each string is equal to that weight (ie the mass, times g). :wink:
 
Viru.universe said:
0k i know net force on a body is defined as mass times acceleration of the body w.r.t inertial frame,
but how do we define individual forces acting on the body?
Eg. Forces acting on a 1kg block are F1=+6¡ And F2=-4¡
So we know net force=2¡, and net acceleration=2 m/s^2
but how do we actually apply something called "6 N" force in right direction, and "4 N" in left direction?
Thank you.
Are you seeking a definition of the individual forces or just wanting to know how a constant force can be applied?

It is easy to imagine such constant forces in a static system. But it is not so easy to explain HOW such constant forces would be applied in a dynamic system.

The 4N force could be friction, which is always opposite to the direction of motion and is fairly constant regardless of speed. But the 6N force would have to be from something like a spring whose extension is maintained as the body accelerates.

AM
 
Yeah i am seeking definition for individual forces, i got examples how to apply constant force to a system
 
There are two sides to the equation. Force is not really defined as mass times acceleration. F = ma is really a definition of mass. ma goes on the left side of the equation, while, on the right side of the equation, you have the net force. This is the sum of all the "contact forces" on the body. A contact force is caused by the mechanical interaction of bodies that are pressing against one another or pulling on one another. Another kind of force is "body force" such as gravity, which also goes on the right side of the equation. GMm/r2 is regarded as a contributor to the acceleration. But ma in not equal to GMm/r2, unless gravity is the only force acting on the body.
 
I didn't understand
"F=ma is really a definition of mass"
 
Viru.universe said:
Yeah i am seeking definition for individual forces, i got examples how to apply constant force to a system
The individual force, F, if applied to an inertial body of mass m on which no other forces were acting, would cause that body to accelerate at a rate of a = F/m. That is how the force would be measured.

We define the concept of force in general terms. F = ma is not necessarily a definition of force. Force is defined in Newton's first law as that which is required to effect a change in the motion of a body. That is the definition of force. F = ma is a formula for determining the magnitude of the force.

Newton observed that the same push or pull applied for equal amounts of time to bodies of different mass caused equal changes in motion in each body, provided one defined the quantity of motion as the body's mass x its velocity. So it seems reasonable to define the magnitude of a force by the magnitude of the changes in motion its causes per unit time: F = dp/dt

AM
 
Viru.universe said:
I didn't understand
"F=ma is really a definition of mass"

Newton determined empirically that the acceleration of a body is proportional to the force applied to the body. Mass is the proportionality constant between the net force on a body and its acceleration. therefore, F=ma can be looked upon as a definition of the property of mass.
 
F = ma (Newton's second law) is not actually the original equation.

The original equation is I = ∆(mv), or impulse = change in momentum

Differentiating that gives dI/dt = ma + (dm/dt)v,

and if m is constant then the RHS is just ma.

We call dI/dt "force", and write it "F"

∆(mv) is easy to measure, and therefore so is I.

a is not so easy to measure (especially in equilibrium! :rolleyes:)​
 

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