Alphabeta Math
LemmaStatement: AI-adaptedProof: AI-generated
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The asymptotic metric flux of Kerr equals its mass parameter

Statement

The ADM energy of the specified constant t Kerr end exists and equals EADM=M.

Facts & Assumptions

[F1]

The following exact suppliers supply the geometric objects and earlier conclusions used here: Asymptotic mass and axial angular-momentum conventions The Boyer–Lindquist spatial end and differentiated expansion

Proof

**Given:**The ADM metric-flux convention and the differentiated expansion of [F1].

Goal: Evaluate the energy flux.

1.1givenF1

Put kij=2Mxixj/r3. Direct differentiation in dimension three gives ∂jkij=2Mxi/r3 and ∂ikjj=−2Mxi/r3. Thus their difference contracted with ni is 4M/r2. The O2(r−2) remainder of the metric contributes O(r−3) to this contracted integrand.

2.1givenF1step 1.1∎

Integration over a Euclidean coordinate sphere gives ∫Sr4M/r2 dS0=16πM. The integrated remainder is O(r−1) and vanishes. Division by 16π and the limit in the definition yield EADM=M.

External input

The cited Kerr coordinate formulas provide background for the local calculation in this item.

Depends on

Used by · 2

Dependency tree · 2 levels

Each result is drawn at its shortest distance from this item. Arrows run from prerequisites to the items that use them; this item has a heavier outline. External source nodes link directly to the cited text. The view shows up to two dependency steps; open a prerequisite to continue.

External dependencies

The Kerr Metric · §2, equations (2.1), (2.5)–(2.8), PDF pp. 2–3

The review gives ingoing and Boyer–Lindquist Kerr forms, their coordinate transformation, and the asymptotic identification of mass M and angular momentum J=aM.

Hypotheses: The Kerr metric in the stated coordinate systems and their indicated domains.

Reading limits: Read the cited formulas and surrounding discussion. This is background for the Kerr construction, not a proof of the full indexed statement or its normalization-specific calculations.

Sources