Quick Jump:

Inertia
  
Angular momentum about center of mass of a rigid body
    Inertia about the center of mass of a rigid body
    Example: finding the inertia of an irregular shaped rigid body
    Example: finding the inertia of a cuboid model of the upper arm

Practical considerations
   
Physical interpretation of the equations of dynamics
    Estimating the inertial parameters of the human arm
    How hard is it to move something twice as fast?

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Angular momentum about center of mass of a rigid body

 

 

Recall that: Torque is the rate of change of angular momentum.

To define inertia, we need to be able to write angular momentum (a vector) in terms of something (inertia, which is a matrix) that multiplies angular velocity.

 

 

 

 

Note that the inertia matrix, when written about the center of mass, is always symmetric.

 

The object shown here is flat and thin.  It is made of aluminum and weighs 19 grams, and is uniform.  Our task is to find its center of mass and its inertia about its center of mass.
  Divide up the piece into equal size squares of 1x1 cm.
  Each small square is assumed to be a particle of mass 1 with its location specified by the center of square.

Size of the upper arm:  32.5x10x7.5 cm
density:  1.05 g/cm3
“particle” size:  2.5x2.5x2.5 cm

When the object is rotating at its center of mass:

When rotation is occurring about another point on the object:

Inertia remains symmetric even if we express it about a point other than center of mass.
Mass appears linearly in all expressions of inertia.
When the body is rotating, the vector sxc will have to be written in terms of angular position of the body with respect to the point of rotation.  Therefore, Is will be a function of position of the body.
 

 

 

 

 

 

 

Example:  Effect of interaction torques
Command a flexion torque on the elbow

Torque on the elbow causes motion of the elbow and shoulder

 

Example:  Effect of interaction torques
Command an extension torque on the elbow

Command a flexion torque on shoulder

 

1.  Immobilize the second link.

Inertia seen by the first joint when the second joint is immobilized.
Reaches maximum value when the arm is open.
2.  Immobilize the first link.

Reaction forces acting on the first link when the second link accelerates.
3.  Centripetal forces acting on link 2 due to rotation of link 1

 

 

Objective:  Is there a simple relation between torques when the speed of movements scales up?
Example:  Imagine that one makes a movement from point 1 to 2 in 1 second.  How much more joint torque would be needed to make the same movement in 0.5 seconds?
 

To move twice as fast, you’d need four times as much torque to compensate for inertial dynamics