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Electric motor scaling laws and inertia in robot actuators

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Why This Matters

This article explores the fundamental principles of robot actuator scaling, emphasizing how motor size impacts torque, inertia, and power dissipation. Understanding these scaling laws is crucial for designing efficient, high-performance robotic systems that balance power, weight, and responsiveness. Such insights help industry professionals optimize actuator selection and improve robot capabilities across various applications.

Key Takeaways

This is the beginning of a series of posts about robot actuation. The intent here is not to prescribe some specific architecture or solution, but to talk about the fundamentals, with as little bias as I can manage. Hopefully you learn something.

Here’s an ostensibly straightforward question for anyone who’s spent time thinking about robot actuators. Take a look at the three cartoon actuators below. One has a large, direct-drive motor, one has a medium-sized motor with a single-stage gear reduction, and the third has a small motor with a a two-stage reduction. The gear ratios are chosen so that the actuators can all produce the same output torque, and all have the same resistive dissipation in the motor for a given output torque. Assume the gears are massless and 100% efficient.

Which of these actuators has the lowest reflected inertia? Defined as the rotor inertia times gear ratio squared.

We’ll come back to this.

First order motor scaling

How do torque, $\tau$, mass, $m$, power dissipation, $p$, and rotor inertia, $j$, scale with motor size? For this analysis, we’ll assume the radial thickness of the stator & rotor is a constant.

First, what happens if only the length, $l$, changes, keeping the current density in the windings constant (equivalent to keeping the magnetic shear pressure constant)? This is pretty intuitive – double the length of the motor, and torque should double, rotor inertia should double, and power dissipation should double (ignoring end-turns): $$\tau, m, p, j \propto l$$

What if only the radius, $r$, changes, again keeping current density in the windings constant?

$$m, p\propto r$$ $$\tau \propto r^{2}$$ $$j\propto r^{3}$$

A simple figure of merit

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