Skip to main content

Posts

Showing posts from 2026

Why I Wrote The Sheet Mechanic (And Why Calculations Aren’t Enough)

For engineers who already know the math—but still lose projects. For the last few years, I’ve been sharing technical guides here on Mechanical Design Handbook —how to size a motor, how to calculate fits, and (as you recently read) how to choose between timing belts and ball screws. But after 25 years in industrial automation, I realized something uncomfortable: Projects rarely fail because the math was wrong. They fail because: The client changed the scope three times in one week. A critical vendor lied about a shipping date (and no one verified it). The installation technician couldn’t fit a wrench into the gap we designed. University taught us the physics. It didn’t teach us the reality. That gap is why I wrote my new book, The Sheet Mechanic . This is not a textbook. It is a field manual for the messy, political, and chaotic space between the CAD model and the factory floor. It captures the systems I’ve used to survive industrial projec...

Stop trying to be a hero. Start being a mechanic.

Get the book →

The Sheet Mechanic on Amazon. Affiliate link, I earn from qualifying purchases.

Flexible Shaft Couplings: Misalignment Is Not Free

Demonstration: Two horizontal shafts rotating together via a jaw-type elastomeric coupling. The Visual Hook vs. Operating Reality The demonstration video linked above presents a clean, elementary mechanical action: two coaxial horizontal shafts rotating steadily together through a jaw-type elastomeric coupling. The assembly features two metallic hubs—each equipped with protruding cast or machined jaws—interlocked through a central elastomeric insert, commonly termed a spider (visible in orange). Visually, the system appears effortless: the shafts appear nearly coaxial and rotate smoothly under demonstration conditions. However, machine designers must be cautious not to read phenomena into an isolated benchtop clip that are not physically displayed. The video is intentionally simple. It does not visibly demonstrate angular misalignment, parallel offset, dynamic backlash, shock absorption, bearing-load reduction, or coupling failure. It serves only as...

Compression Spring Design: Force, Energy, and Limits

In mechanical design, the helical compression spring is often treated as a trivial catalog component. We drop an off-the-shelf CAD model into an assembly, assume a linear restoring force, and move on. Yet when high-speed automated machinery experiences intermittent jamming, erratic seating, or premature fatigue fractures, the root cause frequently traces back to an oversimplified understanding of spring mechanics. Consider the simple physical interaction captured in the short clip below. A bare helical compression spring is positioned upright, compressed downward a small fraction of its free length by manual pressure, and then released. The video demonstrates the most fundamental behavior of a compliant mechanical element: an applied axial displacement generates an immediate opposing reaction force, and removing the constraint allows the stored elastic energy to return the component to its original geometry. The demonstration is intentionally mi...

Nine Moving Links, One Crank: Understanding 1-DOF Motion

At first glance, it almost looks organic. The repeating motion resembles a person performing squats, or a stylized bipedal mechanism flexing through a rhythmic cycle. Behind that visual impression is a deterministic planar mechanism: nine moving links driven by a single continuously rotating crank, coupled through multiple interconnected closed loops. Nine moving links coordinated by a single input crank, simulated in MechanicSim2D. An intuitive reaction to seeing so many moving members is to assume that high link counts create chaotic or under-constrained motion. In kinematics, the opposite is often true: joints impose geometric constraints, and closed loops can reduce the number of independent coordinates when those constraints are independent. Advertisement Planar Mobility: The Kutzbach Criterion with Nine Moving Links In mechanism design, an unconstrained rigid body in planar space has three i...

Simple Harmonic vs Cycloidal Cam Motion: Which Is Smoother?

Two cam motion laws can produce exactly the same lift through exactly the same rise angle at exactly the same camshaft speed—and still behave very differently dynamically. Consider a follower rise bounded by dwells. Compare simple harmonic motion (SHM) with cycloidal motion using the same lift h , rise angle β , and constant camshaft speed ω . Which is smoother? The short answer: cycloidal motion gives better continuity at the dwell boundaries, but it does not produce lower kinematic peaks. For the same lift, rise angle, and cam speed, cycloidal motion has about 27.3% higher peak velocity and 27.3% higher peak acceleration than SHM. Normalize the Cam Rise First Let the normalized cam coordinate during the rise be u = θ / β ,    0 ≤ u ≤ 1 The comparison below assumes an ideal translating follower, constant camshaft angular velocity, and a dwell immediately before and after the rise. Advertisement Simple ...