Physics Asked by MakeItGreatAgain on July 29, 2021
I am working on fundamental dynamics in last few days. The question is about Pfaffian constraint.
A general form of Pfaffian constraint is
$$ A(q)^{mathrm{T}}d{q} + b(q)dt = 0tag{1}$$
which is formed as
$$ A(q)^{mathrm{T}} delta q = 0tag{2}$$ with variation theorem, i.e. $$b(q)dt=0.tag{3}$$
However, in some applications such as non-holonomic system, that the Pfaffain form is simply given by
$$A(q)^{mathrm{T}}dot{q} = 0.tag{4}$$
I simply want the detailed derivation of this form. After searching internet, I didn’t find too much things helpful to the derivation of this form.
The semi-holonomic/Pfaffian constraint (1) is equivalent to $$ A(q)^{mathrm{T}}dot{q} +b(q)~=~ 0;tag{1'} $$ not eq. (4).
However, when considering d'Alembert's principle, time is frozen $$delta t~=~0,$$ so that an infinitesimal virtual displacement $delta q$ satisfies eq. (2).
Answered by Qmechanic on July 29, 2021
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