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Equation 78 · The Bend an Elevator Cannot Fake

What does this equation mean?

ds2=−U(x)2 dx02+δij dxidxjds^2 = -U(\mathbf x)^2\,dx_0^2 + \delta_{ij}\,dx^i dx^j

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Inputs and operations-U(mathbf x)^2dx_0^2 + delta_ijdx^i dx^j
Result or conditionds^2
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

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dd

Symbol d

d is part of the quantity the equation computes from the expression on the right.

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s2s^2

Symbol s^2

The square of s: multiply s by itself.

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UU

Symbol U

U is one of the signed contributions combined to compute the quantity on the left.

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xx

Symbol x

x is one of the signed contributions combined to compute the quantity on the left.

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x02x_0^2

Symbol x_0^2

x02x_0^2 is one of the signed contributions combined to compute the quantity on the left.

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δij\delta_{ij}

Symbol delta_ij

deltaia_ij is one of the signed contributions combined to compute the quantity on the left.

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xix^i

Symbol x^i

xix^i is one of the signed contributions combined to compute the quantity on the left.

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xjx^j

Symbol x^j

xjx^j is one of the signed contributions combined to compute the quantity on the left.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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addition

addition

Add the term after the plus sign to the term or group before it.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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superscript

superscript

A raised number can be a power. When it is a label or bound, it selects a case or the upper limit of a sum; the formula’s structure distinguishes these uses.

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How to interpret it

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What the article says around this equation

What must therefore vanish, identically, is not the slope but the correctly defined curvature-frame component built from it. For any static metric of the form ds2s^2 = -U(x\mathbf x)^2\,dx02x_0^2 + δij\delta_{ij}\,dxix^i dxjx^j — flat spatial slices, all the position dependence carried by U — the only nonzero Christoffel symbols are Γ0i0\Gamma^0_{0i} = ∂i\partial_i ln⁡\ln U = ϕ,i\phi_{,i} and Γ00i\Gamma^i_{00} = U2U^2ϕ,i\phi_{,i} , both following directly from the metric’s definition. Substituting into the Riemann tensor’s defining combination for the mixed component RiR^i{}_{0j0} , every term built from purely spatial Christoffels vanishes because the spatial slices are exactly flat, and the two surviving pieces are…
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What must therefore vanish, identically, is not the slope but the correctly defined curvature-frame component built from it. For any static metric of the form ds2s^2 = -U(x\mathbf x)^2\,dx02x_0^2 + δij\delta_{ij}\,dxix^i dxjx^j — flat spatial slices, all the position dependence carried by U — the only nonzero Christoffel symbols are Γ0i0\Gamma^0_{0i} = ∂i\partial_i ln⁡\ln U = ϕ,i\phi_{,i} and Γ00i\Gamma^i_{00} = U2U^2ϕ,i\phi_{,i} , both following directly from the metric’s definition. Substituting into the Riemann tensor’s defining combination for the mixed component RiR^i{}_{0j0} , every term built from purely spatial Christoffels vanishes because the spatial slices are exactly flat, and the two surviving pieces are ∂j\partial_jΓ00i\Gamma^i_{00} and -Γ0λi\Gamma^i_{0\lambda}Γj0λ\Gamma^\lambda_{j0} . Expanding ∂j(U2ϕ,i)\partial_j(U^2\phi_{,i}) = U2U^2ϕ,i\phi_{,i}ϕ,j\phi_{,j} + U2U^2ϕ,ij\phi_{,ij} and Γ00i\Gamma^i_{00}Γj00\Gamma^0_{j0} = U2U^2ϕ,i\phi_{,i}ϕ,j\phi_{,j} , the two copies of ϕ,i\phi_{,i}ϕ,j\phi_{,j} cancel exactly, leaving

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