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Robotic Arm Joint Torque Solution

Formulas & Definitions

In industrial automation and robotics, multi-axis robotic arms manipulate heavy tools and end-effectors in 3D manufacturing space. Robotics and computer systems engineers calculate cross-product torque vectors at each articulated joint to drive servomotor controllers and prevent structural overload.

A 6-axis industrial robot has its base shoulder joint pivot located at the Cartesian origin (0,0,0)(0, 0, 0)(0,0,0). When holding an end-effector welding tool, the position vector from the shoulder pivot to the tool's center of mass is rβƒ—=⟨0.8,0,0.6⟩ meters\vec{r} = \langle 0.8, 0, 0.6 \rangle\text{ meters}r=⟨0.8,0,0.6⟩ meters. The gravitational downward weight of the tool exerts a constant vertical force vector Fβƒ—=⟨0,βˆ’100,0⟩ Newtons\vec{F} = \langle 0, -100, 0 \rangle\text{ Newtons}F=⟨0,βˆ’100,0⟩ Newtons.

  1. Compute the structural torque vector τ⃗=r⃗×F⃗\vec{\tau} = \vec{r} \times \vec{F}τ=r×F experienced at the shoulder pivot joint using a matrix determinant.
  2. Calculate the magnitude of the torque (βˆ£Ο„βƒ—βˆ£|\vec{\tau}|βˆ£Ο„βˆ£) in Newton-meters (Nβ‹…m\text{N}\cdot\text{m}Nβ‹…m).
  3. Identify which Cartesian axes experience bending/torsion moments.

Step-by-Step Solution:

  1. Calculate the Torque Vector (Ο„βƒ—\vec{\tau}Ο„): Set up the 3Γ—33 \times 33Γ—3 matrix determinant:

    Ο„βƒ—=rβƒ—Γ—Fβƒ—=∣i^j^k^0.800.60βˆ’1000∣\vec{\tau} = \vec{r} \times \vec{F} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 0.8 & 0 & 0.6 \\ 0 & -100 & 0 \end{vmatrix}Ο„=rΓ—F=​i^0.80​j^​0βˆ’100​k^0.60​​
    Expand along the top row:
    Ο„βƒ—=i^(0β‹…0βˆ’0.6β‹…(βˆ’100))βˆ’j^(0.8β‹…0βˆ’0.6β‹…0)+k^(0.8β‹…(βˆ’100)βˆ’0β‹…0)\vec{\tau} = \hat{i}(0\cdot 0 - 0.6\cdot (-100)) - \hat{j}(0.8\cdot 0 - 0.6\cdot 0) + \hat{k}(0.8\cdot (-100) - 0\cdot 0)Ο„=i^(0β‹…0βˆ’0.6β‹…(βˆ’100))βˆ’j^​(0.8β‹…0βˆ’0.6β‹…0)+k^(0.8β‹…(βˆ’100)βˆ’0β‹…0)
    Ο„βƒ—=i^(0βˆ’(βˆ’60))βˆ’j^(0βˆ’0)+k^(βˆ’80βˆ’0)\vec{\tau} = \hat{i}(0 - (-60)) - \hat{j}(0 - 0) + \hat{k}(-80 - 0)Ο„=i^(0βˆ’(βˆ’60))βˆ’j^​(0βˆ’0)+k^(βˆ’80βˆ’0)
    Ο„βƒ—=60i^+0j^βˆ’80k^=⟨60,0,βˆ’80⟩ Nβ‹…m\vec{\tau} = 60\hat{i} + 0\hat{j} - 80\hat{k} = \langle 60, 0, -80 \rangle\text{ N}\cdot\text{m}Ο„=60i^+0j^β€‹βˆ’80k^=⟨60,0,βˆ’80⟩ Nβ‹…m

  2. Compute Torque Magnitude (βˆ£Ο„βƒ—βˆ£|\vec{\tau}|βˆ£Ο„βˆ£):

    βˆ£Ο„βƒ—βˆ£=602+02+(βˆ’80)2=3600+0+6400=10000=100Β Nβ‹…m|\vec{\tau}| = \sqrt{60^2 + 0^2 + (-80)^2} = \sqrt{3600 + 0 + 6400} = \sqrt{10000} = 100\text{ N}\cdot\text{m}βˆ£Ο„βˆ£=602+02+(βˆ’80)2​=3600+0+6400​=10000​=100Β Nβ‹…m

  3. Moment Analysis by Axis:

    • xxx-axis moment: +60Β Nβ‹…m+60\text{ N}\cdot\text{m}+60Β Nβ‹…m (pitch bending moment caused by the zzz-displacement of the tool).
    • yyy-axis moment: 0Β Nβ‹…m0\text{ N}\cdot\text{m}0Β Nβ‹…m (no yaw moment since force is parallel to the yyy-axis).
    • zzz-axis moment: βˆ’80Β Nβ‹…m-80\text{ N}\cdot\text{m}βˆ’80Β Nβ‹…m (roll bending moment caused by the xxx-displacement of the tool).

Meaning of the Answer & Real-Life Application:

The joint experiences a total resultant rotational torque of 100Β Nβ‹…m100\text{ N}\cdot\text{m}100Β Nβ‹…m. Robotic control software uses real-time vector cross product calculations based on forward kinematics to calculate joint torques continuously, supplying the exact motor holding current needed to hold poses steady and prevent mechanical joint slippage.