constraints and types of constraints
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Types of constraints
1. Holonomic Constraints:
If all constraints of the system can be expressed as equations having the form f(q1,q2,....., qs) = 0 or their equivalent, then the system is said to be holonomic and the constraints are holonomic constraints.
Example:
* If there’s a sphere or circle of radius a, such that a particle is bound to move on its boundary
We have
r=a
Or r-a= 0
In other words,
f(q1,q2,.....,qs) = 0
Such a constraint is called holonomic constraint.
* A cylinder rolling without slipping down a rough surface inclined at an angle a.
* A horizontal cylinder of radius a rolling inside a perfectly rough hollow horizontal cylinder of radius b>a.
2. Non-holonomic constraint
If the particle cannot move in the boundary or cannot move up to radius distance, we can say
r does not equal 0
Or r-a is not equal to 0.
Also, we can write r<a.
Such constraints are called non-holonomic. Here,
f(q1,q2,.....,qs) does not equal 0
For example,
A sphere constrained to roll on a perfectly rough plane.
A sphere rolling down from the top of a fixed sphere.
Scheleronomic Constraint:
This constraint is independent of time. For example, if a simple pendulum has an inextensible length. In other words, its length does not change as time changes.
Rheonomic Constraint:
This constraint is dependent on time. For example, if the length of the pendulum changes with time, the constraints are Rheonomic.
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