- #1
Kashmir
- 468
- 74
Goldstein 3rd ed says
"First consider holonomic constraints. When we derive Lagrange's equation from either Hamilton's or D'Alembert's principle, the holonomic constraint appear in the last step when the variations in the ##q_i## were considered independent of each other. However, the virtual displacements in the ##\delta q_{I}##'s may not be consistent with constraints. If there are ##n## variables and ##m## constraint equations ##f_\alpha## of the form Eq. (1.37), the extra virtual displacements are eliminated by the method of Lagrange undetermined multipliers.
I do not understand the parts that the virtual displacements may be inconsistent with constraints because earlier on in the book he defines virtual displacement as the infinitesimal change of the coordinates *consistent with the forces and constraints imposed on the system at the given instant ##t##* (pg 16).
"First consider holonomic constraints. When we derive Lagrange's equation from either Hamilton's or D'Alembert's principle, the holonomic constraint appear in the last step when the variations in the ##q_i## were considered independent of each other. However, the virtual displacements in the ##\delta q_{I}##'s may not be consistent with constraints. If there are ##n## variables and ##m## constraint equations ##f_\alpha## of the form Eq. (1.37), the extra virtual displacements are eliminated by the method of Lagrange undetermined multipliers.
I do not understand the parts that the virtual displacements may be inconsistent with constraints because earlier on in the book he defines virtual displacement as the infinitesimal change of the coordinates *consistent with the forces and constraints imposed on the system at the given instant ##t##* (pg 16).