The Complete Guide to Designing and Building a Cycloidal Gear Reducer for Precision Robotics
The cycloidal gear reducer is often considered the mechanical ‘holy grail’ for robotic joint actuation — delivering zero backlash, extreme torque density, and high reduction ratios in a single compact stage.
Unlike common planetary gearboxes, which suffer from inherent backlash and lower torque density per unit volume, a well-designed cycloidal drive stands in a class of its own. The engineering community has long recognized this mechanism as the gold standard for applications where precision, repeatability, and load capacity are non-negotiable requirements.
This guide provides a comprehensive, step-by-step engineering breakdown for designing a professional-grade cycloidal reducer. We will cover the mandatory mathematical foundation, CAD design logic, and critical assembly considerations, using the architecture of the Arctos Robotics ecosystem as our reference model. If you are aiming to build precision automation, this is the technology you must master.
Distributed multi-lobe contact eliminates the clearances that cause backlash in conventional gear trains.
A single disc stage achieves ratios that would require multiple planetary stages to replicate.
At any given instant, approximately half of all ring pins are in simultaneous load-bearing contact.
The distributed contact geometry provides exceptional resistance to sudden overloads.
⚙ Understanding the Cycloidal Principle
A cycloidal reducer (often called a ‘cycloid drive’) transmits power not through interlocking teeth, but through a unique ‘rolling’ mechanism. A single, precisely shaped lobed disc is driven eccentrically within a ring of stationary fixed pins.
To understand this motion, visualize a disc slightly smaller than a ring of marbles. As the disc is pushed from the center by an eccentric cam on the input shaft, it “wobbles” around the interior of the pin ring, forcing the stationary pins to roll along its profiled edge. For every full “wobble” (one complete eccentric rotation of the input shaft), the disc itself rotates forward by only one lobe position.
This seemingly simple mechanism has a profound consequence: if your disc has 10 lobes and the ring has 11 fixed pins, then 10 complete rotations of the input shaft produce only one complete rotation of the disc — a 10:1 reduction in a single stage.
“For every full wobble, the disc rotates forward by exactly one lobe position — producing enormous reduction ratios with negligible internal clearance.”
More critically, this design enables multiple lobes to be in constant, simultaneous engagement with the fixed pins, distributing force across a large contact area and virtually eliminating the backlash inherent in traditional gear trains where only one or two teeth mesh at any moment.
FIG. 1 — Conceptual diagram of the cycloidal rolling principle. The eccentric input drives the disc in a wobbling orbit; contact is distributed across roughly half the pin ring at all times.
Mathematical Parameters & Initial Design
You cannot simply freehand the profile of a cycloidal disc; it must be generated mathematically to function. Before you open any CAD software, you must define four fundamental variables. Getting these numbers wrong — or choosing incompatible combinations — will result in a drive that either cannot be manufactured, or that fails almost immediately in service.
This section is the most critical in the entire guide. Every decision downstream — bearing selection, housing geometry, output pin sizing, lubrication — flows from these initial parameters. Treat this as the specification phase of an engineering project, not a casual sketching session.
1 Fundamental Variables
The entire architecture of the gearbox hinges on the four choices listed below. Study the reference geometry carefully before committing to any specific values.
| Symbol | Parameter | Description | Typical Range |
|---|---|---|---|
| L | Disc Lobes | Number of lobes on the cycloidal disc profile. Directly defines the output reduction ratio. | 6 – 100 |
| P | Ring Pins | Number of stationary pins in the outer housing ring. Standard practice: P = L + 1. | 7 – 101 |
| e | Eccentricity | Offset radius of the input cam from the gearbox centerline. Defines the ‘wobble’ amplitude and is the single most sensitive dimension in the entire design. | 0.5 – 5 mm |
| Rr | Pin Radius | Radius of each individual stationary ring pin. Affects torque capacity and profile curvature. | 1 – 12 mm |
| R | Pitch Circle Radius | Distance from the gearbox center to the centerline of each fixed ring pin. This is the primary size parameter of the gearbox. | 15 – 200 mm |
The Reduction Ratio Formula
Using the industry standard convention of $P = L + 1$, the reduction ratio $i$ is beautifully simple:
With $P = L + 1$, the denominator simplifies to 1, so $i = L$. A 10-lobe disc in an 11-pin ring yields a 10:1 reduction. A 50-lobe disc in a 51-pin ring yields a 50:1 reduction — all in the same compact footprint.
For a single stage in a robotic joint application, ratios of 50:1 to 80:1 are common targets. A 50:1 stage allows a relatively small, high-speed, low-torque servo motor to output substantial holding and working torque at the joint. This is often sufficient to eliminate the need for a secondary gear stage entirely.
FIG. 2 — Engineering reference diagram. This establishes the core geometric logic: P = L + 1, the measurement of the R Pitch Circle, and how eccentricity (e) drives the entire system. Understanding these constraints is mandatory before proceeding.
2 The Lobe Profile Equation
Once your variables ($L$, $P$, $R$, $e$, and $Rr$) are set, you can calculate the $X$ and $Y$ coordinates for the disc’s intricate edge profile. You cannot draw this curve freehand or by eye — you must generate it parametrically. The following parametric equations are the mathematical heart of the entire design:
Where the contact angle $\psi$ is derived from:
The parameter $\phi$ sweeps from $0$ to $2\pi$ radians. By calculating $(X(\phi), Y(\phi))$ at hundreds of closely spaced values of $\phi$, you generate a dense point cloud that, when connected, traces the precise cycloidal disc profile.
Implementing the Profile in CAD
In Fusion 360, SolidWorks, or any professional CAD package, use the Equation Driven Curve (or Spline through Points) tool:
Define your chosen variables ($L$, $P$, $R$, $e$, $Rr$) in the CAD software’s parameter manager or a linked spreadsheet. Using parametric variables — rather than hard-coded numbers — will be invaluable when you need to iterate on your design.
Paste the $X(\phi)$ and $Y(\phi)$ equations into the Equation Driven Curve dialog. Set $\phi$ from $0$ to $2\pi$. The software will sample the curve at many points and generate a smooth spline.
Verify visually that the curve is smooth, closed, and that the lobes have the expected count and form. Any kinks, cusps, or self-intersections at this stage indicate a mathematical error or — more likely — a top-cutting condition (see below).
Extrude the closed profile to your desired disc thickness. As a rule of thumb, disc thickness should be at least $2 \times Rr$ for adequate bending stiffness, and often $3 \times Rr$ for high-load robotics applications.
Fusion 360’s Script & Add-In environment (Python API) is an excellent route for generating high-density point arrays from the equations above. A short Python script can compute 2000+ points and insert them as a fitted spline, giving a far smoother result than the built-in equation curve tool with its limited sample count.
3 Critical Pro-Tip: Avoiding Top-Cutting
This is the most common failure mode for engineers designing a cycloidal disc for the first time, and it is worth dedicating special attention to it.
If your eccentricity ($e$) is too large relative to the Pitch Circle Radius ($R$) and Pin Radius ($Rr$), the lobes will become excessively sharp. The parametric equations will produce a curve that crosses itself — a condition called top-cutting (or self-intersection). A top-cut profile is not just aesthetically wrong: it is physically non-functional. The disc will bind against the pins in the self-intersecting regions and the drive will seize immediately.
To guarantee a smooth, manufacturable, non-self-intersecting curve, always ensure:
$e < \dfrac{R}{P}$
This single inequality is your primary sanity check before exporting any geometry for manufacturing. If your chosen parameters violate it, reduce $e$, increase $R$, or reduce your lobe count.
| Condition | Profile Result | Outcome |
|---|---|---|
| $e \ll R/P$ | Smooth, well-formed lobes | Ideal — proceed to manufacturing |
| $e \approx R/P$ | Lobes become pointed at tips | Marginal — increased pin stress; consider reducing $e$ |
| $e > R/P$ | Self-intersection / top-cutting | Non-functional — redesign required |
Design of Key Components and Sub-Assemblies
With the mathematical master profile complete and verified, you can begin the physical CAD modeling of the three main functional parts. Each part must be designed with the others in mind — the cycloidal drive is an integrated system, and tolerances stack across every interface.
1 The Input Mechanism: The Eccentric Shaft
The input shaft — driven by your electric motor — must include an eccentric cam. This cam, offset from the shaft centerline by exactly the eccentricity value $e$, is the heart of the drive’s function. It is what transforms the continuous rotation of the motor into the characteristic wobbling orbital motion of the cycloidal disc.
The eccentric cam sits inside the central bore of the cycloidal disc. Since the disc wobbles while the cam rotates, there is relative motion between the cam surface and the disc bore. This relative motion must be handled by a high-quality bearing — not by direct sliding contact, which would cause catastrophic wear within hours.
Bearing Selection for the Eccentric Cam
In precision systems like those from Arctos Robotics, this interface uses one of two bearing types:
- →Needle Roller Bearings: Exceptionally thin radial section; ideal when you need to minimize the bore diameter of the disc and maximize the wall thickness around the output holes. High radial load capacity for their size. Preferred in high-ratio, high-load designs.
- →Standard Deep Groove Ball Bearings: Available in a wider range of off-the-shelf metric sizes. Lower radial load capacity per unit volume, but easier to source and replace. Suitable for lower reduction ratios and lighter-duty designs.
In high-precision variants, the entire shaft may be machined as a single-piece unit from alloy steel, with the eccentric cam formed integrally. Alternatively, a precisely ground eccentric sleeve can be pressed or shrink-fitted onto a standard ground shaft. Either approach must result in the cam offset being held to ±0.005 mm or better — any error here feeds directly into output position error.
FIG. 3 — Input mechanism detail. The eccentric cam (offset by dimension e) drives the disc in its orbital path. Needle roller bearings at the cam interface minimize friction and wear.
2 Power Extraction: The Output Mechanism
The defining engineering challenge of a cycloidal reducer is this: the disc wobbles while it rotates, but your output shaft must spin smoothly without wobble. You need a mechanism that extracts only the pure rotational component of the disc’s complex motion.
This is accomplished using a system of Output Pins and Holes (also referred to as Roller Pins in the literature).
Output Holes in the Disc
A ring of large circular holes is machined directly into the cycloidal disc, arranged symmetrically around the central bore. These holes are visible in all cross-section reference images of cycloidal drives. The number of output holes is a design parameter, but is typically 4–8 for a small gearbox, up to 12 or more for a large one. More holes means better torque distribution and lower stress on each individual pin.
Output Pins in the Flange
Cylindrical pins, mounted to a separate output flange (or to the housing cover, depending on your architecture), pass through these holes. As the disc wobbles and rotates, the pins, which are fixed to the output flange and cannot wobble, ride around the inside of the holes. The reaction force they exert on the hole walls is what drives the flange to rotate.
The Critical Clearance Relationship
The diameter of the output holes ($D_h$) must be precisely larger than the diameter of the output pins ($D_{pin}$) by exactly twice the eccentricity:
This $2e$ clearance is not a tolerance — it is an exact geometric requirement. The disc must be free to trace its full eccentric orbit ($e$ in every direction from center) around each output pin. Too little clearance and the pins will bind in the holes; too much and the drive will exhibit backlash — the very problem you are trying to eliminate.
The disc is free to wobble in its eccentric orbit around each pin, but the pins themselves constrain the disc’s rotation relative to the output flange. The result is that the output flange receives only the pure rotational component of the disc’s motion — the wobble is mechanically filtered out.
FIG. 4 — Output kinematics detail. This diagram is pivotal: it isolates the single output hole and roller pin to illustrate the specific gap (2e) required to accommodate the disc’s eccentric wobble while transmitting pure rotation to the output flange.
3 Output Stage Architecture and Housing
With the core moving parts modeled, the supporting structure must be designed. This is not merely a shell — the housing is a precision load-bearing component that must maintain exact geometry under the substantial radial forces generated during operation.
Disc Duplication — Counter-Balancing
A single cycloidal disc, by nature of its eccentric motion, generates a rotating imbalance force. At high input speeds this creates vibration, noise, and accelerated bearing wear. The solution used in virtually all professional cycloidal drives is to duplicate the disc.
Two identical cycloidal discs (often labeled D1 and D2 in assembly drawings) are mounted on the eccentric shaft at 180° out of phase with each other. This means when D1 is at its maximum positive eccentricity offset, D2 is at its maximum negative offset. The imbalance forces cancel, vibration drops dramatically, and both discs share the transmitted load — effectively doubling the torque capacity of the stage.
The two-disc arrangement also improves the smoothness of power transmission. Because the two discs are phased opposite to each other, one disc is always approaching maximum pin engagement while the other is retreating, creating a more continuous torque output curve.
Housing Design Considerations
The gearbox housing must feature precisely machined pockets or bores to receive the stationary ring pins. The key design requirements are:
- →Rigidity: The housing walls must be thick enough to resist deflection under radial pin loads. Finite Element Analysis (FEA) is recommended for any housing intended for real-world duty. As a practical guideline, the wall section around the pin pockets should be at least equal to $R_r$ in thickness.
- →Pin Retention: The fixed ring pins must be rigidly located and prevented from rotating or moving axially. Common approaches include pressing pins into blind bores, using snap rings, or capturing pins between two housing halves (R and L covers).
- →Alignment: The left (L) and right (R) housing covers must align the pin ring and bearing bores to within microns. Precision dowel pins are the standard approach; do not rely on fastener clearance holes for alignment.
- →Sealing: The housing must retain lubricant and exclude contamination. O-ring grooves at the mating faces and shaft seals at the input and output are the minimum requirement for any industrial application.
FIG. 5 — Definitive cross-section. The eccentric input shaft drives both cycloidal discs (180° out of phase). Power is extracted via the output roller pins. The dual-disc arrangement cancels imbalance forces and doubles torque capacity.
Assembly & Kinematics Check
A cycloidal gearbox is only as precise as its construction. Even the most perfectly designed profile will not operate correctly without meticulous assembly and lubrication. The Arctos Robotics assembly manual images provide the definitive visual reference for how these complex components come together.
1 Kinematics of the Drive
Before committing to physical assembly, it is worth running through the full kinematic chain on paper (or in simulation) to verify that your design is correct:
Input rotation: The motor drives the eccentric shaft. One full rotation of the shaft moves the eccentric cam through one complete orbit of radius $e$ around the shaft centerline.
Disc wobble: The cam bearing transmits this orbital motion to the cycloidal disc. The disc wobbles in a circle of radius $e$, while simultaneously being constrained by the fixed ring pins to rotate slowly in the opposite direction.
Disc rotation: For each complete orbit (one motor revolution), the disc advances by one lobe pitch in the reverse direction. After $L$ motor revolutions, the disc has completed exactly one full reverse rotation.
Output extraction: The output roller pins, riding in the disc’s output holes with clearance $2e$, pick up only the slow reverse rotation and transfer it to the output flange — with the orbital wobble mechanically cancelled by the clearance geometry.
Output shaft: The output flange rotates at $1/L$ of the input speed, in the opposite direction to the input, delivering the full amplified torque to the load.
In your CAD assembly, mate the eccentric shaft and verify that the disc lobes correctly envelope the pin ring through a full rotation. Any collision or gap indicates an error in the profile equations or parameter entry. Modern CAD tools with motion simulation (Fusion 360 Motion Study, SolidWorks Motion) can animate this kinematic chain before you cut any metal or print any parts.
2 Critical Assembly Considerations
The dual-disc mechanism is standard in high-precision robotics to maximize stiffness, distribute radial loads across two sets of pin contacts, and eliminate the imbalance vibration that a single disc would produce. The assembly sequence below reflects best practice for a two-disc cycloidal stage.
Tolerance and Fit Requirements
The tolerance stack in a cycloidal drive is unforgiving. Every component interface contributes to the total error budget. The table below summarizes the key fits:
| Interface | Recommended Fit | Consequence of Error |
|---|---|---|
| Fixed pin to housing bore | H6/k5 (interference to light press) | Pin movement → disc binding, accelerated wear |
| Eccentric bearing OD to disc bore | H7/k6 (light press) | Bearing spin in bore → rapid failure |
| Eccentric bearing ID to shaft | k5/h5 (transition to interference) | Shaft-bearing slip → fretting, vibration |
| Output pins to flange bores | H6/n5 (interference) | Pin wobble → backlash, noise |
| Main output bearing to housing | H7/k6 | Bearing misalignment → shortened life |
| Output hole diameter ($D_h$) | $D_{pin} + 2e ± 0.005$ mm | Clearance error → binding or backlash |
Needle Bearings on the Eccentric Shaft
High-performance designs like the Arctos Robotics variant rely heavily on needle roller bearings at the eccentric cam interface. These thin-section bearings offer an outstanding radial load-to-size ratio, which is critical here because:
- →The eccentric cam OD is a direct dimension of the input shaft, which must be kept as small as possible to leave room for the disc profile and output holes.
- →Radial loads at the cam bearing are very high — they are the reaction to the full torque being transmitted through the disc lobes. A full complement needle bearing (without a cage) maximizes the rolling element count and thus the load capacity within the limited bore.
Lubrication Requirements
Lubrication is not optional — it is as much a part of the design as the geometry itself. The rolling contacts between the disc lobes and ring pins, and between the cam and the disc bore bearing, operate under extreme Hertzian contact stress. The following guidelines apply:
- GREASEHigh-quality lithium-complex NLGI #2 grease is the standard choice for sealed gearboxes. Apply generously to all pin contacts, cam bearing, and output pin/hole interfaces before first run. Re-lubricate per the manufacturer’s interval, or at minimum annually for robotic arm applications.
- OILCirculating or splash oil lubrication is used in high-speed industrial variants. This approach provides active cooling in addition to lubrication and is preferred when input speeds exceed approximately 2000 RPM.
- AVOIDDry running, even briefly, is fatal to cycloidal drives. Never conduct run-in testing without full lubrication applied. The high contact pressures will cause surface pitting within minutes of dry operation.
Step-by-Step Build Reference
Follow these stages sequentially during your own assembly process. Each stage corresponds to a reference image from the Arctos Robotics assembly documentation. Study the image carefully before proceeding to the next stage.
Input & Housing Prep
Study the gearbox cross-section. Understand the fixed pin positions, eccentric shaft geometry, and roller pin arrangement before touching any components.
Main Components
Verify your 3D printed or machined cycloidal disc against the isolated disc drawing. Check lobe count, output hole diameter, and central bore size before assembly.
Dual Disc & Structure
Install both discs on the eccentric shaft, ensuring the 180° phase relationship is correct. Install needle bearings, phase the discs, and fit the housing covers.
↗ Stage 1: Input and Housing Preparation
Reference: Cycloidal Gearbox Cross-Section (1:2 scale)
This is the core architectural overview. Study it carefully before touching any components. It defines how power is transferred from input to output, and shows the spatial relationship between every component in the assembled gearbox. Key things to identify:
- The fixed ring pins and their housing pockets
- The eccentric shaft centerline offset relative to the housing centerline
- The roller (output) pins and their relationship to the output flange
- The main input and output bearing positions
FIG. REF-A — Core architectural overview at 1:2 scale. Study this before assembly to internalize the spatial relationships between all components.
↗ Stage 2: Main Components
Reference: 3D CAD Line Drawing — Single Cycloidal Disc
This drawing isolates the 3D form of the cycloidal disc. Use it to verify your modeled or manufactured geometry against the reference. Check:
- Lobe count matches your $L$ parameter exactly
- Output hole count and diameter ($D_h = D_{pin} + 2e$)
- Central bore diameter matches the eccentric bearing OD
- Disc thickness is sufficient for the expected load
- No top-cutting or sharp cusps visible on the lobe tips
FIG. REF-B — Isolated 3D view of the cycloidal disc. Cross-reference this against your own geometry before committing to manufacturing.
↗ Stage 3: Dual Disc Assembly and Structure
Reference: Y Gearbox Exploded View
This exploded view is critical for understanding the assembly logic. It shows how the two cycloidal discs are stacked on the dual-cam eccentric shaft with the correct 180° phase offset. Key assembly points visible in this image:
- The dual-cam eccentric shaft with cams at 180° offset
- Needle roller bearings at each cam (one per disc)
- The phase-shifted dual-disc stack (D1, D2)
- Main housing structure (R and L covers) and their alignment features
- Output roller pins connecting the disc assembly to the output flange
FIG. REF-C — Exploded assembly view. The 180° phase offset between the two eccentric cam positions is clearly visible here. This is the key assembly detail that ensures balanced, vibration-free operation.
Advanced Assembly & Precision Tuning
Once the core assembly is complete and verified dimensionally, the final step involves setting the bearing preload. This is a critical step that cannot be overstressed — and it is the step that most separates a hobbyist build from a professional-grade precision instrument.
1 Understanding Preload
Bearing preload refers to the internal axial load applied to a bearing during installation — typically by means of spacers, shims, or a precision nut — that eliminates internal radial and axial clearance (known as ‘free play’ or ‘end play’) within the bearing itself.
The consequences of incorrect preload are severe in a cycloidal drive:
Rolling elements and raceways are under constant internal stress. Operating temperature rises sharply. Bearing life may be reduced to a fraction of rated values. The drive may feel ‘stiff’ or resist back-driving.
Free play in the bearings allows the output shaft to move without the input moving — directly defeating the core purpose of the cycloidal drive. The output will ‘float’ under reversing loads.
2 Preload Setting Procedure
Clean all bearing seats and bores before final assembly. Even fine swarf or lint can cause a false preload reading. Use isopropyl alcohol and clean lint-free cloths.
Select your shim/spacer stack. Based on your housing measurements and bearing specifications, calculate the initial shim thickness. Start conservative (slightly under preloaded) — it is easier to add preload than to disassemble a seized drive.
Torque the retaining hardware to the specification in the assembly manual. Do not estimate by feel — use a calibrated torque wrench. Fastener torque directly determines the preload delivered to the bearing through the spacer stack.
Check rolling resistance. With all fasteners at spec, rotate the input shaft by hand. The drive should spin smoothly with a consistent, moderate resistance. There should be no tight spots, grinding, or binding. There should also be zero detectable angular play at the output with the input held stationary.
Run-in procedure. Before putting the drive into service, run it unloaded at 25% rated speed for 30 minutes, then check for abnormal heat (above approximately 60°C is a concern). Then run at 50% speed for 30 minutes and repeat the heat check. This allows the lubricant to distribute fully and surfaces to micro-conform, establishing the initial wear surface.
Final verification. After run-in, conduct a backlash check using a precision dial indicator at the output flange with the input locked. Total indicated movement should be less than 1 arc-minute (0.017°) for a well-built precision drive. Arctos Robotics targets sub-arc-minute performance on their standard gearbox designs.
When tuned correctly, a well-built cycloidal drive exhibits virtually zero backlash, very smooth and consistent motion, and a characteristic that makes it especially valuable in robotics: back-driveability. A back-driveable joint can be moved by external force without damaging the gearbox — essential for collision safety in collaborative robots and for easy manual teaching of robot paths.
3 Comparing Cycloidal to Alternatives
| Attribute | Cycloidal Drive | Planetary Gearbox | Harmonic Drive | Worm Gear |
|---|---|---|---|---|
| Backlash | ~Zero | Low–Medium | ~Zero | Medium–High |
| Torque Density | Very High | Medium | High | Medium |
| Shock Load Capacity | Excellent | Good | Poor (flex spline) | Fair |
| Single-Stage Ratio | 10:1 – 120:1 | 3:1 – 15:1 | 30:1 – 320:1 | 5:1 – 100:1 |
| Back-Driveability | Yes | Yes | Yes | Generally No |
| Manufacturing Complexity | High | Medium | Very High | Low–Medium |
| Cost (at equivalent ratio) | Medium–High | Low–Medium | Very High | Low |
The cycloidal drive’s combination of zero backlash, high torque density, excellent shock capacity, and back-driveability makes it the preferred choice for collaborative robot joints, surgical robots, and high-precision automation — wherever position accuracy and safety under unexpected loads are paramount.
Downloads & Further Resources
Ready to study a working model or build your own? The Arctos Robotics Y Gearbox is a high-performance design, optimized for 3D printing and standard metric bearings, and it utilizes the exact principles outlined throughout this guide.
↓ Download the Cycloidal Gearbox Model
The complete files for the Arctos Robotics Y Gearbox are available for free download on Printables. The package includes all STL and STEP files for the cycloidal discs, housing covers, eccentric shaft (for machining reference), and output flange. Whether you intend to study the geometry in CAD or print and build a working unit, these files are the fastest route from theory to hardware.
📖 Official Assembly Manual
For the detailed, multi-page instructions used to build the complete robotic joint — including specific bearing part numbers, torque settings, shim selection tables, alignment checks, and run-in procedures — refer to the official Arctos Robotics Assembly Manual (Beta). This document is the authoritative reference for all assembly dimensions referenced in this guide.
🤖 Explore Arctos Robotic Arms
While building your own gearbox is a fundamental and deeply rewarding learning experience, achieving consistent industrial-grade precision across a full six-axis arm requires specialized manufacturing processes, precision metrology equipment, and rigorous quality control — resources that are difficult to replicate in a typical workshop or makerspace.
The Arctos Robotic Arm kits utilize these exact cycloidal gearbox principles — featuring high reduction ratios, robust dual-disc architecture, and precision-ground components — to achieve repeatable sub-millimeter positioning in a desktop form factor. Each joint in the arm is an iteration of the exact design methodology covered in this guide.
Read more
How to Get Started in Robotics: The No-Nonsense Guide to Building a Pro-Level Portfolio
How to Get Started in Robotics: The No-Nonsense…
Robotic Arm Design: Principles, Components, and the Arctos Approach
Robotic Arm Drawing: From Concept Sketches to CAD…
Robotic Arm Design: Principles, Components, and the Arctos Approach
Robotic Arm Design: Principles, Components, and the Arctos…
Can I Do Robotics Without Coding? Exploring No-Code Pathways
Can I Do Robotics Without Coding? Exploring No-Code…