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Equation 8 · The Valley of Stability Is a Fitness Landscape

What does this equation mean?

B(A,Z)=aVA−aSA2/3−aCZ(Z−1)A1/3−aA(A−2Z)2A+δ(A)B(A,Z) = a_V A - a_S A^{2/3} - a_C \frac{Z(Z-1)}{A^{1/3}} - a_A \frac{(A-2Z)^2}{A} + \delta(A)

Read the formula alongside the article passage below. Each part has a deeper page with its role in the equation, the supporting passage and nearby citations.

Start withZ(Z-1)
Divide byA^1/3
This relates toB(A,Z)
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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BB

Symbol B

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

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AA

Symbol A

A is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.

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ZZ

Symbol Z

the mass number.

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aVa_V

Symbol a_V

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

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aSa_S

Symbol a_S

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

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A2/3A^{2/3}

Symbol A^2/3

A2A^2/3 is one of the signed contributions combined to compute the quantity on the left.

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aCa_C

Symbol a_C

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

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A1/3A^{1/3}

Symbol A^1/3

A1A^1/3 occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

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aAa_A

Symbol a_A

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

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δ\delta

Symbol delta

delta 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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fraction

fraction

Divide the expression above the line by the one below it.

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addition

addition

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

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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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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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Z(Z−1)Z(Z-1)

Numerator: Z(Z-1)

The complete quantity above the fraction bar.

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(A−2Z)2(A-2Z)^2

Numerator: (A-2Z)^2

The complete quantity above the fraction bar.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction. Read it with the definitions, units, and assumptions supplied by the article.

What the article says around this equation

The quantity that plays fitness’s role has a name in nuclear physics already: binding energy per nucleon, B(A,Z)/A , where A = N + Z is the mass number. It is the energy that would have to be supplied to disassemble a nucleus into Z free protons and N free neutrons, divided by the number of nucleons, and a higher value means a more tightly bound, lower-energy configuration — precisely the sense in which a fitness function assigns a scalar payoff to a state. The theoretical account of how that payoff varies across the chart is the semi-empirical mass formula, first written down by Carl Friedrich von Weizsäcker in 1935 as a liquid-drop model of the nucleus [ 11 ] . In one common form, the…
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The quantity that plays fitness’s role has a name in nuclear physics already: binding energy per nucleon, B(A,Z)/A , where A = N + Z is the mass number. It is the energy that would have to be supplied to disassemble a nucleus into Z free protons and N free neutrons, divided by the number of nucleons, and a higher value means a more tightly bound, lower-energy configuration — precisely the sense in which a fitness function assigns a scalar payoff to a state. The theoretical account of how that payoff varies across the chart is the semi-empirical mass formula, first written down by Carl Friedrich von Weizsäcker in 1935 as a liquid-drop model of the nucleus [ 11 ] . In one common form, the binding energy is B(A,Z)=aVA−aSA2/3−aCZ(Z−1)A1/3−aA(A−2Z)2A+δ(A)B(A,Z) = a_V A - a_S A^{2/3} - a_C \frac{Z(Z-1)}{A^{1/3}} - a_A \frac{(A-2Z)^2}{A} + \delta(A). with a pairing term commonly written

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Sources cited in the surrounding passage

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