Difference between revisions of "Force"

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Force is defined as rate of change of [[momentum]] of a body (F = dp/dt). A unit of force is the[[newton]].
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'''Force''' is defined as rate of change of [[momentum]] of a body ('''F''' = dp/dt). The [[International System of Units|SI]] unit of force is the [[newton]] and the [[US customary system]] unit is the pound.
  
The momentum is given by ''p = m v''. For non-[[Theory of Relativity|relativistic]] speeds, ''F = m a''.<ref>Marcelo Alonso and Edward J. Finn, ''Fundamental University Physics'', Addison-Wesley.</ref> In these expressions, ''F'' stands for the total vector sum of all forces, ''m'' for the mass of the object, ''a'' for its [[acceleration]] expressed as a vector, ''p'' stands for momentum vector  and ''v'' for velocity vector.  
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The momentum of an object is given by ''p = m v''. For non-[[Theory of Relativity|relativistic]] speeds, ''F = m a''.<ref>Marcelo Alonso and Edward J. Finn, ''Fundamental University Physics'', Addison-Wesley.</ref> In these expressions, ''F'' stands for the total vector sum of all forces, ''m'' for the mass of the object, ''a'' for its [[acceleration]] expressed as a vector, ''p'' stands for momentum vector  and ''v'' for velocity vector.  
  
 
There are four known fundamental types of forces occurring in nature<ref>Lewis H. Ryder, ''Quantum Field Theory'', 2nd ed., Cambridge University Press, Cambridge (UK), 1996</ref>:
 
There are four known fundamental types of forces occurring in nature<ref>Lewis H. Ryder, ''Quantum Field Theory'', 2nd ed., Cambridge University Press, Cambridge (UK), 1996</ref>:
  
 
;[[Electromagnetism|Electromagnetic]] force
 
;[[Electromagnetism|Electromagnetic]] force
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:The force that acts on objects with [[electric charge]].
 
;[[Gravitation]]al force
 
;[[Gravitation]]al force
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:The force that attracts any two objects with [[mass]].
 
;Strong force
 
;Strong force
:this is the force that keeps [[atom]]ic [[nucleus|nuclei]] together.
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:The force that keeps [[atom]]ic [[nucleus|nuclei]] together.
 
;Weak force
 
;Weak force
:this force is (amongst other things) involved in ''beta decay'', in which a [[neutron]] in an atomic nucleus is changed to a [[proton]], emitting an [[electron]] and a [[neutrino]].
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:This force is involved in ''beta decay'', in which a [[neutron]] in an atomic nucleus is changed to a [[proton]], emitting an [[electron]] and a [[neutrino]].
  
It should be noted that the latter two forces have an extremely short range (on the order of femtometers), and that a classical (Newtonian or relativistic) description of these forces is not possible. They can only be desribed using [[quantum field theory]], a relativistic version of [[quantum mechanics]].
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It should be noted that the latter two forces have an extremely short range (on the order of femtometers), and that a classical (Newtonian or relativistic) description of these forces is not possible. They can only be described using [[quantum field theory]], a relativistic version of [[quantum mechanics]].
  
 
==References==
 
==References==

Revision as of 19:50, July 30, 2007

Force is defined as rate of change of momentum of a body (F = dp/dt). The SI unit of force is the newton and the US customary system unit is the pound.

The momentum of an object is given by p = m v. For non-relativistic speeds, F = m a.[1] In these expressions, F stands for the total vector sum of all forces, m for the mass of the object, a for its acceleration expressed as a vector, p stands for momentum vector and v for velocity vector.

There are four known fundamental types of forces occurring in nature[2]:

Electromagnetic force
The force that acts on objects with electric charge.
Gravitational force
The force that attracts any two objects with mass.
Strong force
The force that keeps atomic nuclei together.
Weak force
This force is involved in beta decay, in which a neutron in an atomic nucleus is changed to a proton, emitting an electron and a neutrino.

It should be noted that the latter two forces have an extremely short range (on the order of femtometers), and that a classical (Newtonian or relativistic) description of these forces is not possible. They can only be described using quantum field theory, a relativistic version of quantum mechanics.

References

  1. Marcelo Alonso and Edward J. Finn, Fundamental University Physics, Addison-Wesley.
  2. Lewis H. Ryder, Quantum Field Theory, 2nd ed., Cambridge University Press, Cambridge (UK), 1996