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Kashmir
- 468
- 74
I dont Understand how we get the final equations relating ##Q_r## with ##\lambda## given the conditions above?
Lagrange Equations in the context of non-holonomic systems are a set of differential equations that describe the motion of a system subject to constraints that are not integrable into conditions on the coordinates alone. These constraints typically involve the velocities of the system and cannot be expressed purely as functions of the coordinates.
Non-holonomic constraints depend on the velocities and cannot be reduced to constraints on the coordinates alone, making them non-integrable. Holonomic constraints, on the other hand, can be expressed as functions of the coordinates and possibly time, and they are integrable.
Lagrange multipliers in non-holonomic systems are introduced to enforce the constraints. They are additional variables that, when included in the Lagrangian formulation, modify the equations of motion to account for the non-holonomic constraints.
To derive the Lagrange Equations for a non-holonomic system, you start with the standard Lagrangian formulation, introduce the non-holonomic constraints using Lagrange multipliers, and then apply the Euler-Lagrange equations. The resulting equations will include terms involving the Lagrange multipliers that enforce the constraints.
An example of a non-holonomic system is a rolling wheel that cannot slip. The constraint is that the velocity of the point of contact with the ground must be zero. For such a system, you would write the Lagrangian considering the kinetic energy of the wheel, introduce the non-holonomic constraint using a Lagrange multiplier, and derive the equations of motion using the modified Euler-Lagrange equations.