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the 1980 edition is the 2nd edition... the 3rd edition was released in 2002.... plus it had two coauthors
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::<math>\mathcal{F}_i= - \frac{\partial \mathcal{V}}{\partial q_i}\, </math> ;
::<math>\mathcal{F}_i= - \frac{\partial \mathcal{V}}{\partial q_i}\, </math> ;


[[Lagrangian mechanics]] often involves monogenic systems. If a physical system is both a [[holonomic system]] and a monogenic system, then it is possible to derive [[Lagrangian mechanics|Lagrange's equation]]s from [[d'Alembert's principle]]; it is also possible to derive [[Lagrangian mechanics|Lagrange's equation]]s from [[Hamilton's principle]].<ref name="Herb1980">{{cite book |last=Goldstein|first=Herbert|title=Classical Mechanics|year=1980| location=United States of America | publisher=Addison Wesley| edition= 3rd| isbn=0-201-65702-3 | pages=18–21, 45}}</ref>
[[Lagrangian mechanics]] often involves monogenic systems. If a physical system is both a [[holonomic system]] and a monogenic system, then it is possible to derive [[Lagrangian mechanics|Lagrange's equation]]s from [[d'Alembert's principle]]; it is also possible to derive [[Lagrangian mechanics|Lagrange's equation]]s from [[Hamilton's principle]].<ref name=goldstein2002>{{cite book |last1=Goldstein |first1=Herbert |authorlink1=Herbert Goldstein |last2=Poole | first2=Charles P., Jr. |last3=Safko |first3=John L. |title=Classical Mechanics |edition=3rd |year=2002 |url=http://www.pearsonhighered.com/educator/product/Classical-Mechanics/9780201657029.page |isbn=0-201-65702-3 |publisher=Addison Wesley |location=San Francisco, CA |pages=18–21,45}}</ref>


==See also==
==See also==

Revision as of 01:06, 29 October 2013

In physics, among the most studied physical systems in classical mechanics are monogenic systems. A monogenic system has excellent mathematical characteristics and is very well suited for mathematical analysis. It is considered a logical starting point for any serious physics endeavour.

In a physical system, if all forces, with the exception of the constraint forces, are derivable from the generalized scalar potential, and this generalized scalar potential is a function of generalized coordinates, generalized velocities, or time, then, this system is a monogenic system.

Expressed using equations, the exact relationship between generalized force and generalized potential is as follows:

where is generalized coordinate, is generalized velocity, and is time.

If the generalized potential in a monogenic system depends only on generalized coordinates, and not on generalized velocities and time, then, this system is a conservative system.The relationship between generalized force and generalized potential is as follows:

Lagrangian mechanics often involves monogenic systems. If a physical system is both a holonomic system and a monogenic system, then it is possible to derive Lagrange's equations from d'Alembert's principle; it is also possible to derive Lagrange's equations from Hamilton's principle.[1]

See also

References

  1. ^ Goldstein, Herbert; Poole, Charles P., Jr.; Safko, John L. (2002). Classical Mechanics (3rd ed.). San Francisco, CA: Addison Wesley. pp. 18–21, 45. ISBN 0-201-65702-3.{{cite book}}: CS1 maint: multiple names: authors list (link)