Jacobians- velocities and static forces Flashcards
How can a(bVq) be represented as a rotation matrix?
a(bVq) = abR x Vq
where lower case letters are super/sub scripts
How can bVq be represented in terms of differentiation?
lim∆t bQ(t+∆t) - bQ(t) / ∆t
How dowe define the rotation of frame {b} relative to frame {a}?
aΩb
how do we represent aΩb mapped to frame {c}?
c(aΩb)
How else can we represent uΩc?
Where u is a universe frame
Wc (omega)
Define aWb
the angular velocity of {b} relative to {universal} expressed in {a}
If we have frames {a} and {b} which are not coincident, how do we represent the linear velocity of bVq in terms of {a}
aVq = a(bVq) + aVb.org
where aVb.org is the velocity of the position vector aPb.org
If frames {a} and {B} are coincident, and we have an angular velocity aΩb and linear velocity bVq, how is aVq defined?
aVq = (aΩb x abRbQ) + abRbVq
In the general case where origins are not coincident, we have aΩb and bVq, how do we find aVq?
aVq = (aΩb x abRbQ) + (abRbVq) + aVb.org
What is the vector cross product of rotational velocity?
aVq = aΩb X aQ
What is the purpose of Jacobians?
It can define cartesian velocities in terms of joint velocities (map from joint to cartesian)
v = J(ø)x ø
How can we find the Jacobian using the partial differentiation method?
- Conduct forward kinematics to get transformation matrix to end effector frame
- Partially differentiate the position vector of the end effector
- Find jacobian using ºv=ºJ(ø)ø
When using partial differentiation how are terms differentiated in terms of øi ?
Terms that do not include øi are cancelled out and terms with øi are differentiated
Identity for cos(ø1 + ø2)
cos(ø1+ø2) - sin(ø1 +ø2) = cos(ø1+ø2)
Identity for sin(ø1 +ø2)
cosø1sinø2 + cosø2+sinø1