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Robotic Manufacturing & CNC Toolpaths Solution

In precision manufacturing and aerospace robotics, automated laser cutters and multi-axis CNC milling tools must trace intricate 3D contoured profiles along metal workpieces. To prevent localized heat buildup, material burning, or excessive tool wear, the cutting head must maintain a perfectly uniform physical feed rate across spatial coordinates, regardless of the mathematical parameterization of the motor drives.

An automated robotic laser cutter at a UNLV advanced manufacturing laboratory traces a cutting path along an aerospace titanium bracket according to the vector position function:

r⃗(t)=⟨13t3,t2,2t⟩\vec{r}(t) = \left\langle \frac{1}{3}t^3, t^2, 2t \right\rangle
where coordinates (x,y,z)(x, y, z) are measured in millimeters and t≥0t \ge 0 represents an internal motor cycle parameter.

  1. State the formula for the accumulated arc length function s(t)s(t) and compute s(t)s(t) starting from initial cycle t=0t = 0.
  2. Invert the arc length function to solve for the motor cycle parameter tt in terms of physical traversal distance ss.
  3. Formulate the intrinsic arc length parametrization r⃗(s)\vec{r}(s) and determine the exact coordinate location of the laser cutter after it has traversed an arc length of s=73 mms = \frac{7}{3}\text{ mm}.

Step-by-Step Solution:

  1. Compute Velocity Vector and Scalar Speed: State the Vector Derivative Formula:

    r⃗′(t)=⟨ddt[13t3],ddt[t2],ddt[2t]⟩=⟨t2,2t,2⟩\vec{r}'(t) = \left\langle \frac{d}{dt}\left[\frac{1}{3}t^3\right], \frac{d}{dt}\left[t^2\right], \frac{d}{dt}[2t] \right\rangle = \langle t^2, 2t, 2 \rangle

    State the Scalar Speed Formula:

    ∥r⃗′(t)∥=(t2)2+(2t)2+22=t4+4t2+4\|\vec{r}'(t)\| = \sqrt{(t^2)^2 + (2t)^2 + 2^2} = \sqrt{t^4 + 4t^2 + 4}
    Notice that the polynomial under the radical is a perfect square trinomial:
    t4+4t2+4=(t2+2)2  ⟹  ∥r⃗′(t)∥=(t2+2)2=t2+2t^4 + 4t^2 + 4 = (t^2 + 2)^2 \implies \|\vec{r}'(t)\| = \sqrt{(t^2 + 2)^2} = t^2 + 2

    State the Arc Length Function Formula:

    s(t)=∫0t∥r⃗′(u)∥ du=∫0t(u2+2) du=[13u3+2u]0t=13t3+2ts(t) = \int_{0}^{t} \|\vec{r}'(u)\|\,du = \int_{0}^{t} (u^2 + 2)\,du = \left[ \frac{1}{3}u^3 + 2u \right]_{0}^{t} = \frac{1}{3}t^3 + 2t

  2. Invert to Solve for tt as a Function of Arc Length ss: Set s=13t3+2t  ⟹  t3+6t−3s=0s = \frac{1}{3}t^3 + 2t \implies t^3 + 6t - 3s = 0. Using Cardano's cubic formula for the depressed cubic t3+6t−3s=0t^3 + 6t - 3s = 0 (where p=6,q=−3sp = 6, q = -3s):

    t(s)=3s2+9s24+83+3s2−9s24+83t(s) = \sqrt[3]{\frac{3s}{2} + \sqrt{\frac{9s^2}{4} + 8}} + \sqrt[3]{\frac{3s}{2} - \sqrt{\frac{9s^2}{4} + 8}}

  3. Formulate Intrinsic Parametrization and Evaluate at s=73 mms = \frac{7}{3}\text{ mm}: The intrinsic arc length parametrization is:

    r⃗(s)=⟨13(t(s))3,(t(s))2,2t(s)⟩\vec{r}(s) = \left\langle \frac{1}{3}(t(s))^3, (t(s))^2, 2t(s) \right\rangle

    For s=73 mms = \frac{7}{3}\text{ mm}, solve s(t)=73s(t) = \frac{7}{3}:

    13t3+2t=73  ⟹  t3+6t−7=0\frac{1}{3}t^3 + 2t = \frac{7}{3} \implies t^3 + 6t - 7 = 0
    Factoring by inspection yields (t−1)(t2+t+7)=0  ⟹  t=1(t - 1)(t^2 + t + 7) = 0 \implies t = 1 (the only real root). Substitute t=1t = 1 into r⃗(t)\vec{r}(t):
    r⃗(1)=⟨13(1)3,(1)2,2(1)⟩=⟨13,1,2⟩ mm\vec{r}(1) = \left\langle \frac{1}{3}(1)^3, (1)^2, 2(1) \right\rangle = \left\langle \frac{1}{3}, 1, 2 \right\rangle\text{ mm}

Meaning of the Answer & Real-Life Application:

By parametrizing the laser cutting trajectory as r⃗(s)\vec{r}(s), the CNC motion controller adjusts the servo cycle times to maintain a constant physical feed rate of 1 mm/s1\text{ mm/s} relative to ss. When s=73 mms = \frac{7}{3}\text{ mm} of titanium has been cut, the toolhead is positioned precisely at (1/3,1,2) mm(1/3, 1, 2)\text{ mm}, preventing over-exposure hotspots and structural micro-cracking in the aerospace bracket.