Putting the Mechanics into Quantum Mechanics

As we explore the frontier of quantum computing, we’re not just grappling with abstract concepts like superposition and entanglement—we’re engineering systems that manipulate light, matter, and energy at their most fundamental levels. In many ways, this feels like a return to analog principles, where computation is continuous rather than discrete.

A Return to Analog Thinking

Quantum systems inherently deal with waves—light waves, probability waves, electromagnetic waves. These are the same building blocks that analog computers once harnessed with remarkable efficiency. Analog systems excelled at handling infinite resolution calculations, where signals like video, sound, and RF were treated as continuous phenomena:

  • Video is light being redirected.
  • Sound is pressure waves propagating.
  • RF is electromagnetic waves traveling from point to point.

The challenge now is: how do we process continuously varying signals at the speed of light, without being bottlenecked by digital discretization?

Light as Information

I often joke that light moves at the speed of light—until it’s put on a network. But in the quantum realm, we’re literally dealing with light as both input and output. That changes the paradigm entirely.

To “put the mechanics into quantum mechanics” means:

  • Designing systems that physically embody quantum principles.
  • Treating light not just as a carrier of information, but as the information itself.
  • Building architectures that process analog signals at quantum scales, leveraging phase, amplitude, and polarization as computational resources.

Engineering Quantum Behavior

In this paradigm, we’re not just simulating quantum behavior—we’re engineering it. Quantum computing isn’t just about qubits flipping between 0 and 1; it’s about manipulating the very nature of reality to perform computation. This requires a deep understanding of both the physics and the engineering required to build systems that operate at the atomic and photonic level.

We’re entering an era where the boundaries between physics, computation, and communication blur. And perhaps, by revisiting the principles of analog computation through the lens of quantum mechanics, we’ll unlock new ways to process information—at the speed of light, and with the precision of nature itself.

The Most Powerful Computers You’ve Never Heard Of

 

The Case of the Conductive Cable Conundrum

I love interesting weird audio problems—the stranger the better! When a colleague reached out with a baffling issue of severe signal loading on their freshly built instrument cables, I knew it was right up my alley. It involved high-quality components behaving badly, and it was a great reminder that even experts can overlook a small but critical detail buried in the cable specifications.

The Mystery of the Missing Signal

My colleague was building cables using Mogami instrument cable (specifically 2319 and 2524) and Neutrik NP2X plugs, both industry-standard choices. The results were perplexing:

  • With Neutrik NP2X plugs: The signal was heavily compromised—a clear sign of signal loading—requiring a massive 15dB boost just to achieve a usable volume.

  • With generic ‘Switchcraft-style’ plugs: The cables functioned perfectly, with no signal loss.

The contradiction was the core of the mystery: Why would a premium connector fail where a generic one succeeded, all while using the same high-quality cable?

The Sub-Shield Suspect: A Deep Dive into Cable Design

The answer lay in the specialized design of the Mogami cable, particularly a feature intended to prevent noise. Most musical instrument pickups, like those in electric guitars, are high-impedance, voltage-driven circuits. This makes them highly susceptible to microphonic noise—the minute voltage generated when a cable is flexed or stepped on.

To combat this, the Mogami W2319 cable specification includes a specialized layer:

Layer Material Details
Sub-Shield Conductive PVC (Carbon PVC) Placed under the main shield to drain away this microphonic voltage.

This sub-shield is designed to be conductive.

The Termination Trap

My colleague’s standard, logical termination procedure was to strip the outer jacket and shield, then solder the hot wire to the tip connector with the inner dielectric butted right up against the solder post. This is where the problem originated.

I theorized that the internal geometry of the Neutrik NP2X plugs—which features a tightly-fitted cup and boot—was the culprit:

“It’s the way it sits in the cups. Sometimes it touches. Like when you put the boot on it goes into compression and jams it right up to the solder cup.”

 

When the cable was compressed by the tight Neutrik boot, the exposed, conductive sub-shield was being pushed into contact with the tip solder cup—creating a partial short circuit to ground (the shield). This resistive path to ground is the definition of signal loading, which robbed the high-impedance guitar circuit of its precious voltage and necessitated the hefty 15dB boost. The generic connectors, by chance, had just enough internal clearance to avoid this fatal contact.

The Professional Solution

The specifications confirm the necessity of a careful strip: Note: This conductive layer must be stripped back when wiring, or a partial short will result.

The fix was straightforward: cleanly peel or strip back the black, conductive PVC layer a small amount, ensuring it cannot make contact with the tip solder cup when the connector is fully assembled. This prevents the short and restores the cable’s proper functionality.

My colleague quickly confirmed the successful result:

“The issue was in fact the conductive PVC layer.”

“fuck yeah, nailed it!”

This experience serves as a powerful reminder that even seasoned professionals must respect the specific design and termination requirements of high-quality components. When troubleshooting audio problems, sometimes the most unusual solution is found not in a faulty part, but in a necessary step that was, literally, not in the wire.

Starrett Analog Gage Amplifier – No 718

ButFeatures

  • Zero set control.
  • Screwdriver adjustment for individual calibration.
  • Resolution: .0001″ (0.010mm) to .000010″ (0.001mm)
  • Range: .003″ (.300mm) to 10.0003″ (10.030mm)
  • Only three switches – one for inch/millimeter, one for fine or coarse resolution & one for polarity.\par
  • Compact size of 8″ x 4-3/4″ x 2″ (200 x 119 x 50mm).
  • 110 volt AC operation (7.5 volt transformer furnished).

 

 

Probe to get:

Starrett 715-1Z – LVDT Lever Type Gage Head

 

Calibration

Beskar 2d2 project planning – check list – Things to do

  1. HEAD
    1. Dome
      1. TOP
        1. Life Form Scanner
          1. Antenna
          2. Signal Processors
          3. Extension arm
        2. Flaps
          1. Periscope
            1. Camera
          2. Top (Pie Panels)
        3. Holographic Projector (Top)
      2. Middle
        1. Radar Eye + Primary Photo Receptor
      3. Bottom
        1. Logic Display Small Front
        2. Processor state inicator
        3. Holographic Projector (Front)
        4. Logic Display Large Rear
        5. Flaps – Sides (Dome Panels)
          1. Sensory Input Head
    2. Neck
      1. Head Rotation Ring (cover)
      2. Head Rotation – Lazy Susan
      3. Motor to spin head
      4. Split Rings
  2. BODY
    1. Chest
      1. Spacecraft linkage data slot (Large Data Port)
      2. Utility Arms – Spacefract linkage and conrol arms
    2. Body Compartments
      1. LEFT
        1. Computer Interface
          1. SCOMP
        2. Application interface
        3. Utility Saw
      2. RIGHT
        1. Grasping Arm
        2. Manipulator Arms
    3. Upper Belly
      1. Power Charge Arm Compartment
      2. Coin Slots (System Diagnostic input receptors)
      3. Torso Diagnostic input receptors
      4. Front Vents
        1. Upper ( Acoustic Signaller)
        2. Lower (System ventilation
      5. Pocket Vent
      6. Restraining Bolt
    4. Lower Belly
      1. Coin Return (Polarity Sink)
      2. Recharge Power Coupler
      3. Heat Exhaust (BTU Exhaust Wave)
      4. Interface Pulse Stabilizers
    5. BACK
      1. Recharge Power Coupler
      2. Coin Return (Polarity Sink)
      3. Interface Pulse Stabilizers
    6. Skirt

      (Durasteel Shell)

      1. Foot Lifter
  3. LEG (Left and Right)
    1. Shoulder
      1. Flange
      2. Shim (Horse Shoe)
      3. Hub
      4. Hydralics
      5. Buttons
      6. Under shoulder detail
      7. Actuating Coupler
    2. Leg
      1. Attitude Booster Turbine
      2. Booster Cover
      3. Leg Strut
    3. Ankle
      1. Bracelet
      2. Wedge
      3. Cylinder
    4. Battery Box
      1. Enclosure
      2. Harnessses
      3. Power bus cables (Hoses)
    5. Foot
      1. Skeleton
      2. Wheel
      3. Half Moon
      4. Front Strip
        1. knurled Hose Fitting
  4. Center Foot

    (Third Tread)

    Retractable

    1. Lifter
    2. Leg
    3. Ankle
      1. Cylinder
    4. Foot
      1. Skeleton
      2. Wheel
      3. Half Moon

 

WTB: An Anvil Stand

Description
This wood anvil stump sits between light, adjustable aluminum legs. Use with the 35-lb. anvil.
• Stump draws vibration of hammer blows away from muscles and joints without dampening their effectiveness on metal; designed to reduce noise.
• Set anvil between the aluminum lugs on the top of the stump and screw down the four corners—no need for chains or other restraints.
• Supports anvil and offers metal-lined receptacles to hold stakes and stitched leather loops for your tools.

Hardinge TT – floating Tap

TT Tap Collets are used in the Hardinge® TT-5/8 and TT-3/4 Tap Holders. These collets are stocked in ANSI (USA) and ISO (England) standards. The ANSI Inch-series tap collets relate to taps manufactured in the United States. Metric collets manufactured in the United States have the same shank sizes as those used for the inch series. The metric collets manufactured to the ISO standard have different shank sizes than the ANSI series metric collets.

0.141  = #0-#6
??? In chuck
0.194 = #10
0.220 = #12
0.255 = 1/4″
0.312 = 1/8″ P
0.323 = 7/16″
0.367 = 1/2″
0.381 =3/8″