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Hand Mk5 Coupling Laws

Coupling variables

We report below a sketch of the finger's kinematics:

Hand Mk5 leverism

The following table describes the finger mechanism's coupling variables of the hand Mk5.

Measure UoM Fingers Description Notes
THUMB INDEX MIDDLE RING PINKY
L0x mm -5.55 -5 -5 -5 -5 X coordinate of first end of leverism Those measurements are taken with respect to a coordinate system located in P0 (joint between the palm and first phalanx)
L0y mm 2.85 4 4 4 4 Y coordinate of first end of leverism Those measurements are taken with respect to a coordinate system located in P0 (joint between the palm and first phalanx)
L1x mm 11.5 24 24 24 19 X coordinate of second end of leverism Those measurements are taken with respect to a coordinate system located in P0 (joint between the palm and first phalanx)
L1y mm 1.5 0.8 0.8 0.8 0.5 Y coordinate of second end of leverism Those measurements are taken with respect to a coordinate system located in P0 (joint between the palm and first phalanx)
P1x mm 20 30 30 30 25 X coordinate of the axis of the joint between first and second phalanx Those measurements are taken with respect to a coordinate system located in P0 (joint between the palm and first phalanx)
P1y mm 1.5 1.5 1.5 1.5 1.5 Y coordinate of the axis of the joint between first and second phalanx Those measurements are taken with respect to a coordinate system located in P0 (joint between the palm and first phalanx)
q0off deg -20.71 -7.54 -7.54 -7.54 -7.54 Angle of the lever ACD respect to the vertical in position 0.
q2bias deg 180 173.35 173.35 173.35 170.54 Angle of L1-P1 respect to the horizontal in position 0.
q1off deg 4.29 2.86 2.86 2.86 3.43 Angle of P1-P0 respect to the horizontal in position 0.
q1bias deg 0 0 0 0 0 Angle of B-P0 respect to the horizontal in position 0. Not drawn in the picture because null.
q0 deg 45.32 78.03 78.03 78.03 78.03 Absolute angle of the lever ACD respect the palm, which has its fulcrum at C and transmits motion to the connecting rod AB by reversing the motion of the cable connected at D.
q1 deg 82.06 90 90 90 90 Absolute angle of the first phalanx with respect to the palm.
q2 deg 68.31 189.2 189.2 189.2 183.31 Absolute angle of the second phalanx with respect to the palm.
beta deg 135.65 82.33 82.33 82.33 80.54 Angle between the line P1-L0 and the horizontal and represents an intermediate step for the calculation of q2.
k mm 17.1 29.18 29.18 29.18 24.25 Connecting rod length L1-L0 (constant).
d mm 20.06 30.04 30.04 30.04 25.04 The distance between the two joints P1-P0 (constant).
l mm 8.5 6.04 6.04 6.04 6.08 The distance between the attachment point L1 of the connecting rod L1-L0 on the second knuckle and the second joint P1 (constant).
b mm 6.24 6.4 6.4 6.4 6.4 The distance between the attachment point L0 of the connecting rod L1-L0 on the palm and the first joint P0 (constant).
h mm - - - - - The distance between the second joint P1 and the connection L0 of the connecting rod on the palm (variable, depends on q1).  Not needed for now
s mm 6.52 5.5 5.5 5.5 5.5 the distance between joint B of the connecting rod A-B and joint P0 (constant).
t mm 13 14.5 14.5 14.5 14.5 The length of the connecting rod A-B.
f mm 6 5.5 5.5 5.5 5.5 The length of the connecting rod A-C.
r mm 7.5 8.5 8.5 8.5 8.5 The length of the connecting rod D-C.
a mm - - - - - The distance between the connecting rod joint A and the joint P0 (variable, depends on q0).  Not needed for now

Coupling Laws

Considering the following quantities:

\[b = \left| L_{0} - P_{0} \right|\]
\[d = \left| P_{1} - P_{0} \right|\]
\[l = \left| L_{1} - P_{1} \right|\]
\[k = \left| L_{1} - L_{0} \right|\]
\[s = \left| B - P_{0} \right|\]
\[t = |A - B|\]
\[f = |A - C|\]
\[r = |D - C|\]
\[h(q_{1}) = \left| P_{1}(q_{1}) - L_{0} \right|\]
\[a(q_{0}) = \left| A(q_{0}) - P_{0} \right|\]
\[P_{1x} = P_{0x} + d\cos\left( q_{1} + q_{1off} \right)\]
\[P_{1y} = P_{0y} + d\sin\left( q_{1} + q_{1off} \right)\]
\[A_{x} = C_{x} + f\cos\left( q_{0} + q_{0off} \right)\]
\[A_{y} = C_{y} + f\sin\left( q_{0} + q_{0off} \right)\]

We have \(q_{2}\) that depends only on the variable \(q_{1}\) through the implicit dependence on \(P_{1}\) and h:

\[q_{2} = \tan^{- 1}\left( \frac{P_{1y}(q_{1}) - L_{0y}}{P_{1x}(q_{1}) - L_{0x}} \right) + \cos^{- 1}{\left( \frac{l^{2} - k^{2} + h^{2}(q_{1})}{2lh(q_{1})} \right) + q_{2bias} - \pi}.\]

The Jacobian that relates the variations of \(q_{2}\) to the variations of \(q_{1}\) is:

\[\frac{\partial q_{2}}{\partial q_{1}} = \frac{1}{2 - \frac{d^{2} - b^{2}}{d^{2} - L_{0} \bullet P_{1}}} + \frac{\left( L_{0x}P_{1y} - L_{0y}P_{1x} \right)\left( l^{2} - k^{2} - h^{2} \right)}{2lh^{3}\sqrt{1 - \left( \frac{l^{2} - k^{2} + h^{2}}{2lh} \right)^{2}}}.\]

The relationship between \(q_{0}\) and \(q_{1}\) is:

\[q_{1} = \tan^{- 1}\left( \frac{A_{y}(q_{0}) - P_{0y}}{A_{x}(q_{0}) - P_{0x}} \right) + \cos^{- 1}{\left( \frac{s^{2} - t^{2} + a^{2}(q_{0})}{2sa(q_{0})} \right) - q_{1bias}}.\]