Newton's Laws are usually stated as follows:
- In the absence of external forces, particles either remain at rest or move in straight lines with constant (nonzero) speed.
- The sum of the forces acting on a particle is equal to its mass times its acceleration ($\sum \vec F = m\vec a$)
- If object $A$ exerts a force $\vec F_{AB}$ on object $B$, then object $B$ exerts a force $\vec F_{BA}=-\vec F_{AB}$ on object $A$.
The standard approach in introductory courses is to note that Newton's first law is just a special case of the second but it's possible to take a different view of things. My preferred statements of Newton's laws (for more discerning audiences, of course) are these:
- There exist frames of reference (called inertial frames) in which particles which are not subject to any external forces either remain at rest or move in straight lines with constant (nonzero) speed.
- In an inertial frame, the sum of the forces acting on a particle is equal to its mass times its acceleration ($\sum \vec F = m\vec a$)
- If object $A$ exerts a force $\vec F_{AB}$ on object $B$, then object $B$ exerts a force $\vec F_{BA}=-\vec F_{AB}$ on object $A$.
Taking this viewpoint, the answer to your question is that Moe is not working in an inertial frame of reference. In Moe's frame, particles which are not subject to any external forces will accelerate, which means that Newton's second law does not apply.
Feynman makes the point that it's possible to do physics in non-inertial frames, but it requires us to add extra terms to Newton's second law. These extra terms look like forces, but they do not have any physical origin (they are not due to interactions with other objects, or with some field). These are often called fictitious forces, pseudo-forces, or non-inertial forces.