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VYPER SPACE / ENGINEERING EXPLORER

From Motion.
To Control.

Explore the design. Build the evidence.

EXPLORE THE FINDINGS

GROUND PROTOTYPE / DESIGN + SIMULATION
NOT BUILT OR PHYSICALLY VALIDATED

SUPPLIED PROTOTYPE / V2

A Design.
A Test Agenda.

A ground-test arm, a rotating magnet and a gimballed aluminum target. The supplied CAD and simulation make the next engineering questions visible. Nothing has been built.

ARM ARCHITECTURE
5 axes
FULL-STRETCH CAD REACH
1.127 m
DEVELOPMENT STATUS
Under review
01 / ISOLATE THE EFFECT

Measure the baseline.

The modeled bearings slow the target even with the magnet off. Compare matched free-decay, static-magnet and rotating-magnet runs before attributing a change to braking.

02 / RESPECT THE GEOMETRY

Clear the whole arm.

The moving ring and yoke restrict access. Some simulated tumbles leave no usable approach; several runs report geometric overlaps despite the magnet head staying clear.

03 / CLOSE THE LOOP

Validate what is sensed.

Two-camera fusion, occlusion handling and the hardware drive interface remain development work. Model-based tracking is not a measured perception result.

REPORT REVIEW & INTERPRETATION

Source and status. These findings review the supplied Detumbler arm v2: design, loads and simulation report, its CAD source and simulation files. This is an internal design-and-simulation package, not a validated publication, physical demonstration or flight result. The website uses the qualifications below where the report overstates the evidence.

Stability times are not an efficacy result. Selected 180-second MuJoCo runs reach the software’s stability threshold after approximately 20–39 seconds. “Stable” means an estimated angular rate below 1 degree per second for more than 2 seconds, not zero motion. The report also describes a magnet-off bearing-friction baseline stopping in approximately 60 seconds. These model outputs do not isolate a magnetic braking benefit; matched baseline runs and physical measurements are needed. Simply subtracting stop times is insufficient.

Overlap samples are not impact events. The reported counts of 18, 1,332 and 165 are geometric safety-overlap samples. Physical collision response is disabled on the target hull, ring and yoke. In case A_roll40_s12, the raw result records 1,081 gimbal overlap samples and 251 arm-link/hull overlap samples. The report’s claim that every overlap was with the stand is incorrect: only the magnet head remained clear of the hull. A clear head alone does not establish a safe arm trajectory.

CAD checking is preliminary. The static checker classifies any fastener-to-part overlap as thread engagement, including overlaps that need separate review. Its zero-interference summary does not certify clearance, assembly fit or manufacturability. HJ2 actuator bolt patterns and cable exits must be confirmed against vendor drawings before fabrication.

Reconcile mass before relying on loads. The selected magnet’s catalog mass is 574.1 g; the CAD accounts for two 245.81 g halves, or 491.62 g. Rotor, head and moving-mass totals, inertias and derived load margins require reconciliation. CAD estimates are not measured assembly properties.

Materials need measurement. Materials are selected to reduce parasitic magnetic interaction. Titanium, carbon composites, stainless pins and brass ballast are not all electrically insulating; the claim that the field only brakes the hull is not established. Characterize coupling in the assembled head and stand.

Model limits. Rotor reaction torque is disabled in the supplied simulation. The applied electromagnetic approximation has no finite-element field validation or measured calibration in this package, and some coefficients are assumed. The replay demonstrates a software run, not validated coupled hardware dynamics.

Integration remains open. Two-camera fusion and gimbal-ring occlusion handling are unfinished. The supplied hardware interface covers serial/simulation paths; a working EtherCAT adapter is still to be implemented and verified. The gimbal’s geometry and balance also limit what can be inferred about free-flight motion.

EARLIER INTERACTIVE CONCEPT

Take the
Controls.

Try the earlier simplified browser model. The supplied v2 CAD and recorded simulation are available in the prototype viewer.

OPEN CONCEPT MODEL

NUMERICAL SIMULATION + ILLUSTRATIVE GRAPHICSNot a validated satellite dynamics simulation.

On a small screen, open the full model for more room.

MODEL SCOPE
WHAT THIS MODEL COMPUTES

The model integrates rigid-body angular motion and uses a local-patch phenomenological drag approximation. Its camera estimate is synthetic; the rendered arm is not a full constrained IK solution. Magnetic rotation is visual and does not drive the torque calculation.

Outputs are simulated, not measured. The display does not establish real stopping times, braking efficacy, tracking accuracy or capture safety. Spacecraft reaction, thermal effects and orbital dynamics are not modeled. Detumbling does not remove the target from orbit.

This earlier model is separate from the supplied v2 ground-rig MuJoCo simulation. Explore the supplied CAD replay →

THE ARCHITECTURE

THREE CONNECTED QUESTIONS.

01 / OBSERVATION

Know
the Motion.

Track a changing viewpoint. Estimate how the target turns. Carry uncertainty into every decision.

CAMERA & STATE ESTIMATION

Intended architecture. Calibrated images and matched features can constrain relative pose. Metric position requires known geometry, scale or an independent depth measurement. Estimating spin also requires accounting for camera and servicer motion.

In the earlier browser model. The camera measurement is synthesized from the simulated truth quaternion with added noise. It is not an image-processing or computer-vision pipeline, and its display does not establish tracking performance.

In the supplied v2 work. The proposed rig has two global-shutter cameras and target markers. Two-camera fusion and ring-occlusion handling remain open development work. Simulation does not establish image-based tracking accuracy.

IMAGE SEQUENCE → RELATIVE STATECONCEPT
A camera observes target features across several framesThe camera's viewing cone points toward a geometric target. Three image frames show changing feature locations. Pose, angular velocity and uncertainty are estimated from the sequence. CALIBRATED CAMERArelative viewpoint FEATUREStracked over time UNCERTAINTYpart of the state SEQUENCE, NOT A SINGLE FRAMEearlierlaterlatest ESTIMATED STATEposition · orientation · angular velocity
Concept diagram. The browser model uses synthetic attitude measurements.

02 / ROBOTIC POSITIONING

Place
the Source.

Bring the magnet to a useful pose. Geometry sets where the arm can reach; interaction physics sets what that pose can do.

ARM GEOMETRY & CONTROL

Intended architecture. A controller requests a source position and orientation. Inverse kinematics would translate that pose into joint angles while respecting reach, joint limits, collision clearance and slew limits.

In the earlier browser model. A two-link arm is rendered alongside Cartesian source motion. This is not a complete constrained inverse-kinematics solver or a validated robot trajectory.

In the supplied v2 work. A five-axis CAD arm drives a ground-rig simulation. The moving ring and yoke constrain approach paths; tested mixed-axis tumbles can prevent a usable approach. The complete swept geometry needs review, beyond the magnet head alone.

DESIRED POSE → ARM GEOMETRYCONCEPT
Arm geometry translates a desired source pose into joint anglesAn articulated arm reaches toward a desired magnet pose. Its reachable envelope, joint angles, clearance region, and the difference between requested and actual poses are indicated. REACH ENVELOPE COLLISION CLEARANCEtarget + swept geometry REQUESTED SOURCE POSEposition + orientation ACTUAL SOURCE POSEtrack the remaining error θ₁θ₂θ₃ IK handles geometry. Braking effectiveness requires a field model.
Concept diagram. Rendered arm motion is distinct from constrained robot kinematics.

03 / MAGNETIC INTERACTION

Change
the Spin.

A changing magnetic field can induce currents in a conducting target. The resulting torque depends on the interaction—not rotation alone.

TORQUE MODEL & LIMITS

Intended architecture. The motor rotates a transverse magnetic dipole so its direction changes. Induced currents interact with the field; torque depends on geometry, material, frequency and relative motion. Arbitrary magnet rotation can add energy.

In the earlier browser model. Angular motion is integrated numerically using rigid-body Euler equations and a quaternion update. Braking comes from a phenomenological local-patch drag model. The displayed magnetic phase does not enter the torque calculation, so the rotating field graphic is illustrative.

In the supplied v2 work. An applied magnetic torque model acts alongside modeled bearing friction. The reported stop times do not isolate magnetic braking. Baseline decay, balance and parasitic coupling need physical characterization. Spacecraft reaction, thermal effects and orbital dynamics are not modeled here; reducing spin does not remove an object from orbit.

FIELD CHANGE → CURRENTS → TORQUECONCEPT
Motor-driven magnet interacts with currents induced in a conducting targetA transverse permanent magnet is attached to a motor shaft beside a conductive target. A changing field induces currents and torque. A feedback path observes the resulting motion and replans the command. NS τ MOTOR COMMANDchoose direction + rate TRANSVERSE DIPOLErotation changes the field INDUCED EDDY CURRENTSinside the conductive target TORQUEsign is model-dependent OBSERVE MOTION → REVIEW ENERGY → REPLANavoid overshoot and unintended spin-up
Concept diagram. The model’s drag approximation is not a solved eddy-current field.

FROM DESIGN TO EVIDENCE

The Next
Experiments.

A staged plan for the proposed ground prototype. These are planned checks, not completed milestones.

PARTS & BUILD PLAN
  1. 01

    Review the design inputs.

    Confirm actuator drawings, magnet mass, tube fits, wiring clearance and rotor containment. Recalculate loads and inspect fastener engagements.

  2. 02

    Characterize the target stand.

    Build and balance the stand first. Measure free spin decay, gravity bias and repeatability before introducing the magnetic source.

  3. 03

    Verify sensing and motion.

    Complete camera fusion and the EtherCAT interface. Test occlusion, retreat paths and whole-arm clearance across the intended gimbal envelope.

  4. 04

    Compare controlled interactions.

    Run matched magnet-off, static and rotating-field experiments. Measure torque, temperature and parasitic effects, with uncertainty and repeat runs.

THE RESEARCH CONTEXT

Build on
What Is Known.

Published work frames the mechanism. Experiments must establish what this prototype can do.

RESEARCH & REFERENCES