← Mathematical compendium

Published equation contexts

RN\mathbf R_N

Why this formula appears here

Start with the least controversial position anyone has ever assigned to an extended body: the Newtonian, mass-weighted centroid, RN\mathbf R_N = ∑a\sum_a mam_a ra\mathbf r_a / ∑a\sum_a mam_a , a sum over the body’s constituent mass elements mam_a at positions ra\mathbf r_a , evaluated at one common instant. That last clause is doing all the work relativity is about to object to. “One common instant” means one value of a time coordinate t shared by every term in the sum — the coordinate time of whichever inertial frame is doing the summing, not any single mass element’s own proper time along its own worldline — and which value of t counts as simultaneous with which is exactly the freedom special relativity…

Read the full article-specific guide →

Read the representative guide

RNR_N

Symbol R_N

RNR_N is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

Read this term in its guide →

How to interpret it

Read this expression with the definitions, units, and assumptions supplied by the article.

Research cited beside this formula

Published contexts (5)

A symbol can carry a different meaning in another article. Each occurrence keeps its own guide and term definitions.

RN\mathbf R_N

Equation 6 · Evolutionary Physics

The Atlas That Refuses to Close

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

Start with the least controversial position anyone has ever assigned to an extended body: the Newtonian, mass-weighted centroid, RN\mathbf R_N = ∑a\sum_a mam_a ra\mathbf r_a / ∑a\sum_a mam_a , a sum over the body’s constituent mass elements mam_a at positions ra\mathbf r_a , evaluated at one common instant. That last clause is doing all the work relativity is about to object to. “One common instant” means one value of a time coordinate t shared by every term in the sum — the coordinate time of whichever inertial frame is doing the summing, not any single mass element’s own proper time along its own worldline — and which value of t counts as simultaneous with which is exactly the freedom special relativity…

Equation guide → · Article →
RN\mathbf R_N

Equation 52 · Evolutionary Physics

The Atlas That Refuses to Close

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

This is the atlas’s first transition function, and it is worth stating exactly what it does and does not compare. It holds the spin supplementary condition — the rule that picks out a unique centroid once an observer is specified — completely fixed, and varies only the observer. It says nothing yet about what happens if the observer is held fixed and the rule itself is changed; that is the next chart’s business. And it comes with two checks for free. First, a conservation check: PμP^\mu and JμνJ^{\mu\nu} , the body’s total four-momentum and total angular momentum, are identical for every observer in this comparison, since they are the Poincaré charges of one physical state and no relabeling of…

Equation guide → · Article →
RN\mathbf R_N

Equation 63 · Evolutionary Physics

The Atlas That Refuses to Close

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

The derivation behind this trade-off runs through the ten generators of the Poincaré algebra rather than through anything special to a particular particle. The boost generator K\mathbf K is one fixed physical object for a given one-particle state; writing it as a symmetrized combination of a position candidate and the energy only closes the algebra’s commutation relations correctly if either the position candidate absorbs a spin-momentum term, yielding commuting components and frame dependence, the Newton–Wigner choice, or that term is left attached to the boost generator itself, leaving the position candidate free of it but noncommuting, the covariant choice. Both are legitimate solutions of…

Equation guide → · Article →
RN\mathbf R_N

Equation 82 · Evolutionary Physics

The Atlas That Refuses to Close

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

What zitterbewegung adds to the atlas is a fourth, sharper illustration of the same structural point as the Pryce trade-off: x^\hat{\mathbf x} and XNW\mathbf X_{\mathrm{NW}} disagree not by a fixed offset but by a time-dependent, oscillating quantity, largest exactly where a wavepacket carries significant negative-energy content, a regime the nonrelativistic limit removes entirely. As v ≪\ll c and the wavepacket is restricted to the positive-energy subspace, the oscillating term’s amplitude falls relative to the packet’s own spatial width, and x^\hat{\mathbf x} , XNW\mathbf X_{\mathrm{NW}} , and RN\mathbf R_N converge onto one description — the same nonrelativistic recovery checked twice already,…

Equation guide → · Article →
RN\mathbf R_N

Equation 113 · Evolutionary Physics

The Atlas That Refuses to Close

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

Collect the pieces. Three charts, the Newtonian centroid RN\mathbf R_N , the observer-dependent stress-energy centroid Xμ(u,Σ)X^\mu(u,\Sigma) , and the canonical Newton–Wigner operator XNW\mathbf X_{\mathrm{NW}} , form a genuine, well-behaved sub-atlas. Define, for any two of them evaluated on the same hypersurface Σ\Sigma ,

Equation guide → · Article →