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Symmetry Principles and Conservation Laws in Atomic and ...

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GENERAL ARTICLEacceleration. Newton's second law conta<strong>in</strong>s the heartof this stimulus{response relation, expressed as a di®erentialequation. It is <strong>in</strong>terest<strong>in</strong>g that laws of classicalmechanics can be built alternatively on the basis of an`<strong>in</strong>tegral pr<strong>in</strong>ciple', namely the `pr<strong>in</strong>ciple of variation',discussed <strong>in</strong> the next section.3. Pr<strong>in</strong>ciple of VariationThe connection between symmetry <strong>and</strong> conservation lawsbecomes even more transparent <strong>in</strong> the alternative formalismof classical mechanics, namely the Lagrangian/Hamiltonian formulation. It is <strong>in</strong>structive to ¯rst seethat this alternative formalism is based not on the l<strong>in</strong>earresponse relationship embodied <strong>in</strong> the Newtonian pr<strong>in</strong>cipleof causality, but <strong>in</strong> a completely di®erent approach,namely the `pr<strong>in</strong>ciple of variation'.It is <strong>in</strong>terest<strong>in</strong>g thatlaws of classicalmechanics can bebuilt alternativelyon the basis of an‘<strong>in</strong>tegral pr<strong>in</strong>ciple’,namely the‘pr<strong>in</strong>ciple ofvariation’,Newtonian mechanics o®ers an accurate description ofclassical motion by account<strong>in</strong>g for the same by the `cause<strong>and</strong> e®ect' relationship. An alternative <strong>and</strong> equivalentdescription makes it redundant to <strong>in</strong>voke such a causaldescription. This alternative description dispenses theNewtonian notion of the 'cause-e®ect' relationship, <strong>and</strong><strong>in</strong>stead of it <strong>in</strong>vokes a variational pr<strong>in</strong>ciple, namely, thatthe `action <strong>in</strong>tegral' is an extremum. Those who are usedto th<strong>in</strong>k<strong>in</strong>g <strong>in</strong> terms of the Newtonian formulation alonewould ¯nd it strange that one gets equivalent descriptionof classical mechanics without <strong>in</strong>vok<strong>in</strong>g the notion offorce at all!Let us ¯rst state the pr<strong>in</strong>ciple of extremum action. Webeg<strong>in</strong> on common ground with the Newtonian formulation,namely that the position q <strong>and</strong> velocity : q specifythe mechanical state of a system. A well-de¯ned functionof q <strong>and</strong> : q would also then specify the mechanicalstate of the system. What is known as the Lagrangian ofa system L(q; : q) is just that; it is named after its orig<strong>in</strong>atorLagrange (1736{1813). Furthermore, <strong>in</strong> a homoge-RESONANCE September 2010835

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