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Equation 1 · What a Biosignature Has to Rule Out

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Φ=G(nobs)−G(neq).\Phi = G(\mathbf{n}_{\mathrm{obs}}) - G(\mathbf{n}_{\mathrm{eq}}).

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Inputs and operationsG(n_obs) - G(n_eq)
Result or conditionPhi
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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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Φ\Phi

Symbol Phi

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

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GG

Symbol G

G 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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subtraction

subtraction

Subtract the following term or group from the preceding one. A leading minus marks a negative quantity.

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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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What the article says around this equation

If no gas can be trusted individually, the natural move is to look for a property of the whole atmosphere. The most general candidate is thermodynamic disequilibrium: life is a persistent chemical engine, so a biosphere should hold its planet’s atmosphere away from the composition it would relax to if all permitted reactions ran to completion. The quantity is the available Gibbs energy — the difference between the free energy of the observed composition and that of its equilibrium state at the same elemental abundances, temperature and pressure: Φ=G(nobs)−G(neq)\Phi = G(\mathbf{n}_{\mathrm{obs}}) - G(\mathbf{n}_{\mathrm{eq}}). Krissansen-Totton, Olson and Catling computed this across Earth history and reported values that make the appeal obvious and…
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If no gas can be trusted individually, the natural move is to look for a property of the whole atmosphere. The most general candidate is thermodynamic disequilibrium: life is a persistent chemical engine, so a biosphere should hold its planet’s atmosphere away from the composition it would relax to if all permitted reactions ran to completion. The quantity is the available Gibbs energy — the difference between the free energy of the observed composition and that of its equilibrium state at the same elemental abundances, temperature and pressure: Φ=G(nobs)−G(neq)\Phi = G(\mathbf{n}_{\mathrm{obs}}) - G(\mathbf{n}_{\mathrm{eq}}). Krissansen-Totton, Olson and Catling computed this across Earth history and reported values that make the appeal obvious and the limitation equally obvious. Earth’s purely gas-phase disequilibrium is small, about 1.5 joules per mole of atmosphere; when the full atmosphere-ocean fluid envelope is included, the figure rises to roughly 2,326 joules per mole, dominated by the coexistence of nitrogen, oxygen and liquid water, which would react to nitric acid at equilibrium. For the maximum Archean case — an anoxic atmosphere in which the disequilibrium is carried by the coexistence of carbon dioxide, nitrogen, methane and liquid water — they obtain about 234 joules per mole [ 2 ] .

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