Jacobians- velocities and static forces Flashcards

1
Q

How can a(bVq) be represented as a rotation matrix?

A

a(bVq) = abR x Vq
where lower case letters are super/sub scripts

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2
Q

How can bVq be represented in terms of differentiation?

A

lim∆t bQ(t+∆t) - bQ(t) / ∆t

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3
Q

How dowe define the rotation of frame {b} relative to frame {a}?

A

aΩb

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4
Q

how do we represent aΩb mapped to frame {c}?

A

c(aΩb)

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5
Q

How else can we represent uΩc?
Where u is a universe frame

A

Wc (omega)

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6
Q

Define aWb

A

the angular velocity of {b} relative to {universal} expressed in {a}

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7
Q

If we have frames {a} and {b} which are not coincident, how do we represent the linear velocity of bVq in terms of {a}

A

aVq = a(bVq) + aVb.org

where aVb.org is the velocity of the position vector aPb.org

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8
Q

If frames {a} and {B} are coincident, and we have an angular velocity aΩb and linear velocity bVq, how is aVq defined?

A

aVq = (aΩb x abRbQ) + abRbVq

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9
Q

In the general case where origins are not coincident, we have aΩb and bVq, how do we find aVq?

A

aVq = (aΩb x abRbQ) + (abRbVq) + aVb.org

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10
Q

What is the vector cross product of rotational velocity?

A

aVq = aΩb X aQ

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11
Q

What is the purpose of Jacobians?

A

It can define cartesian velocities in terms of joint velocities (map from joint to cartesian)
v = J(ø)x ø

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12
Q

How can we find the Jacobian using the partial differentiation method?

A
  1. Conduct forward kinematics to get transformation matrix to end effector frame
  2. Partially differentiate the position vector of the end effector
  3. Find jacobian using ºv=ºJ(ø)ø
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13
Q

When using partial differentiation how are terms differentiated in terms of øi ?

A

Terms that do not include øi are cancelled out and terms with øi are differentiated

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14
Q

Identity for cos(ø1 + ø2)

A

cos(ø1+ø2) - sin(ø1 +ø2) = cos(ø1+ø2)

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15
Q

Identity for sin(ø1 +ø2)

A

cosø1sinø2 + cosø2+sinø1

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16
Q
A