Semi-holonomic constraints (analytical mechanics)

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SUMMARY

Semi-holonomic constraints in analytical mechanics can be expressed in the form fi=(q1,q2,...,qn,\dot{q}1,...,\dot{qn}). A common representation is given by the equation Σaikdqk + aitdt = 0, where aik and ait are coefficients that may depend on the generalized coordinates q and their derivatives \dot{q}. The discussion clarifies that while the two forms of the equations are not equivalent, the second form represents a frequently encountered special case. Understanding these constraints is crucial for analyzing systems in mechanics.

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maria clara
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m equations of semi-holonomic constraints can be put in the form:

fi=(q1,q2,...,qn,\dot{q}1,...,\dot{qn})

but "commonly appears in the restricted form:

\Sigmaaikdqk +aitdt = 0

(i,k,t preceded by "a" should appear in subscript and the sum is over k)

I don't understand this form. what are the coefficients aik and ait? can they be functions of q or q dot?
I don't understand how is it possible for these two equations to be equivalent.
consider for example the following equation of a non-holonomic constraint: q1^2+q2dot=0
what would the second form of this equation look like? :confused:
 
Last edited:
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sorry for the last post (couldn't delete it for some reason)... I was confused, but now I realize the second equation is not exactly equivalent to the first, but represents only a special case which is quite common.
 
maria clara said:
sorry for the last post (couldn't delete it for some reason)... I was confused, but now I realize the second equation is not exactly equivalent to the first, but represents only a special case which is quite common.

I don't think you can delete the first post in a new thread.

Also, have you taken a look at the Latex tutorial? It's an easy way to display equations.
 
now I have, thanks:smile:
 

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