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SCIENCE · INVESTIGATE AND EXPLAIN

Compare fuel inventory with average power

Use reservoir and luminosity comparisons to interpret a conditional support duration.

Learning outcome: Calculate accessible hydrogen and explain why energy divided by power is not a measured lifetime.

Starting recap

Hydrogen fuel is 0.70 times the available-region fraction times the chosen total mass.

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Try

Ten percent at one nominal solar luminosity gives approximately 7.268 Gyr as a budget ratio.

Open the experiment

Predict

What happens if both available region and photon demand double?

Experiment

Compare 10 percent/one unit, 20 percent/one unit and 20 percent/two units; capture the zero-fuel boundary.

Trace fusion energy into a conditional fuel budget

Worked teaching model · synthetic values · Synthetic total mass 2.0×10³⁰ kg; the chosen accessible region has fixed hydrogen-1 mass fraction 0.70. Neutral-atom mass differences include electron bookkeeping. A restricted pp-I mean assigns 0.530 MeV per completion to escaping neutrinos. Remaining energy is assumed to support the specified average photon demand. Rates are required, not achieved; zero fuel supports zero duration. No actual stellar lifetime, reaction-rate, structure, mixing or evolution prediction is made.

Reset keeps your prediction, captures and practice history.

Build helium from hydrogen, then ask how much energy a specified fuel inventory could supply. The two controls change the hypothetical inventory and average photon demand; they do not change nuclear masses or calculate an actual stellar reaction rate.

pp-I worked mechanism · p = proton; n = neutron; e⁺ = positron; νe = neutrinoTwice: p + p → ²H (1p + 1n) + e⁺ + νeTwo weak conversions produce two neutrons and two escaping neutrinos.Twice: ²H + p → ³He (2p + 1n) + γγ denotes a gamma photon. Both intermediate helium-3 nuclei are used next.Once: ³He + ³He → ⁴He (2p + 2n) + p + pSix protons entered the preceding stages; two return. Net consumption: four.Also twice: e⁺ + e⁻ → photons. Surrounding electrons supply the e⁻.Cancel intermediates on paper. This chain is not one four-proton collision.Reaction count does not determine a rate; temperature and density are not modeled.

For the energy ledger, use four neutral hydrogen-1 atoms and one neutral helium-4 atom. This is consistent rest-mass bookkeeping for the net process, not neutral atoms inside the hot core. Four initial electrons account for two in the final atom and two annihilating with positrons. Do not add annihilation rest energy again. Plasma ionization and tiny neutrino rest-mass corrections are omitted.

Rest masses · common scale 0–4.1 u4 neutral H-11 neutral He-40 u4.1 uDifference 0.02869687 u ≈ 0.712% of initial fuel rest mass.Released energy · separate scale 0–27 MeV0 MeV27 MeVDeposited: 26.201 MeV; neutrinos: 0.530 MeV mean.Total: 26.731 MeV. Mass-energy is conserved.

The gold energy segment is the stipulated mean carried away by two pp neutrinos, not a fixed energy for each event or a universal average over all fusion branches. Deposited energy can thermalize before escaping as photons. Nearly all initial fuel rest mass remains in helium.

Hypothetical available inventory and required demand rates
QuantitySelected demandSame inventory, 1 nominal solar luminosity
Accessible region kg2.00000e+292.00000e+29
Hydrogen inventory kg1.40000e+291.40000e+29
Possible net completions2.09138e+552.09138e+55
Helium product rest mass kg1.39003e+291.39003e+29
Total released budget J8.95692e+438.95692e+43
Neutrino budget J1.77591e+421.77591e+42
Deposited budget J8.77933e+438.77933e+43
Prescribed photon demand W3.82800e+263.82800e+26
Required completions per second9.11894e+379.11894e+37
Required hydrogen processing kg/s6.10434e+116.10434e+11
Required rest-mass conversion kg/s4.34538e+94.34538e+9
Implied neutrino power at required rate W7.74338e+247.74338e+24
Conditional support duration Gyr7.267517.26751
Compare independent reservoirs · NOT a stellar time historyConditional support duration (Gyr) · solid/circle selected; dashed/square reference030609012015005101520Available core region (% of synthetic total mass)Hydrogen fraction fixed at 0.70. Long budget ≠ a physically predicted stellar lifetime.

Selected support budget: 7.26751 Gyr; same inventory at the reference demand: 7.26751 Gyr. The two curves coincide because their demands are equal. Each curve compares separate inventories; it does not show a core expanding over time.

Connect fuel, mass difference and power

Let q be the selected region percentage divided by 100. Available hydrogen mass is Mfuel = 0.70 × q × 2.0 × 10³⁰ kg. Count possible net completions as N = Mfuel / (4mH u), with mH = 1.00782503223 and u = 1.66053906892 × 10⁻²⁷ kg. The selected isotope mass differs from a natural-isotope average.

Mass defect per completion is Δm = (4mH − mHe)u, with mHe = 4.00260325413. Released energy is Qtotal = Δm c²; c = 299792458 m/s. Subtract the stipulated mean neutrino energy once: Qdeposit = Qtotal − Qν. One MeV = 1.602176634 × 10⁻¹³ J. Total deposited budget is N Qdeposit.

Divide that energy budget by prescribed average photon luminosity Lγ to obtain a duration in seconds. Divide by 31557600 and one billion to express Gyr. A required completion rate Lγ/Qdeposit is distinct from the amount of fuel. At 10% region and one nominal solar luminosity, 1.40 × 10²⁹ kg of hydrogen supplies about 8.77933 × 10⁴³ J deposited energy, a conditional 7.26751 Gyr budget.

This assumes all deposited energy supports the average photon demand, with no net storage change, mechanical loss or alternate source. Actual stellar temperature, density, mixing, luminosity history and other branches are absent. No present age, remaining lifetime or feasible reaction rate follows from this ratio.

Sources: isotope-specific masses from NIST hydrogen and helium; CODATA conversion constants; Berkeley pp-chain explanation; Fukugita and Peebles on neutrino energy; IAU nominal luminosity. Values use central reference constants without uncertainty propagation; displayed precision is not a new measurement.

Available hydrogen 1.4000e+29 kg; deposited budget 8.7793e+43 J; conditional support duration 7.2675 Gyr.

The prescribed photon demand would require 9.1189e+37 pp-I completions/s and 6.1043e+11 kg/s of hydrogen processing. These are demand-derived required rates, not actual output. The energy/power ratio is not a stellar lifetime prediction.

Captures preserve hypothetical fuel-region and photon-demand choices. Replaying calculates conditional energy budgets and required rates, not measured fusion output or actual stellar lifetimes.

Understand

Separate inventory from power

A reservoir can contain a great deal of usable energy and still be exhausted quickly if the prescribed output is large. This experiment asks how long a stipulated hydrogen inventory could support a stipulated average photon power. It does not calculate a star’s actual lifetime, its remaining age or its present evolutionary stage.

Write two headings on paper: available energy in joules and demanded power in joules per second. Dividing the first by the second gives seconds. Before calculating, predict what happens when only the inventory doubles, then when only the power doubles. These are different comparisons even if both are described loosely as making the star larger or brighter.

Calculate the hydrogen actually available

The hypothetical total stellar mass M is fixed at 2.0 × 10³⁰ kg. It is a chosen round value, not an exact solar mass. The available-region control supplies a percentage a; its fraction is q = a/100. That region initially has hydrogen mass fraction X = 0.70. Hydrogen fuel mass is therefore Mf = XqM.

At the default a = 10, q = 0.10. The available region contains 2.0 × 10²⁹ kg of material, of which 1.40 × 10²⁹ kg is hydrogen fuel. The remaining material is not an additional hydrogen supply. All of the specified hydrogen is assumed convertible through the restricted net chain, with no calculation of mixing or spatial fuel gradients.

Make a three-row ledger for total mass, available-region mass and hydrogen mass. Compare 5, 10 and 20 percent at fixed photon demand. Predict the intermediate quantities before using the lab. A core-region fraction and a hydrogen fraction inside that region are two separate factors, not competing descriptions of the same percentage.

Turn fuel into a conditional duration

From the atomic mass and energy ledger, the deposited energy per kilogram of hydrogen is approximately 6.271 × 10¹⁴ J/kg. Multiplying by the default fuel inventory gives approximately 8.779 × 10⁴³ J. Deposited energy excludes the fixed mean energy escaping in pp neutrinos.

The selected average photon power is a multiple of nominal solar luminosity L₀ = 3.828 × 10²⁶ W, defined in the IAU nominal-constant resolution. For one L₀, duration τ = Edeposit/Lγ is approximately 7.268 billion model years. One displayed year is 31,557,600 seconds. A billion years is one Gyr; it is a unit conversion, not an age determination.

This ratio assumes deposited nuclear energy eventually supports the stated average photon luminosity, without net stored-energy changes, mechanical losses or another energy source. The underlying pp-chain context comes from Lawrence Berkeley National Laboratory. Energy per completed chain does not supply the missing stellar-structure and reaction-rate physics.

Make paired comparisons

At 20 percent and one L₀, available energy and duration double to approximately 14.535 Gyr; the required reaction rate stays fixed. At 10 percent and two L₀, duration halves to approximately 3.634 Gyr while the required rate doubles. Compare each with the reference, which always uses the same selected reservoir and one L₀.

Capture a third case: 20 percent and two L₀. Doubling both reservoir and demand restores the default duration. Equal duration therefore does not imply equal fuel inventory or equal luminosity. Explain the cancellation using a fraction on paper before consulting the calculated result.

The sensitivity chart compares separate budgets across available-region percentages. It is not a time history of a core expanding. Its fixed scale includes the long mathematical duration at 20 percent and 0.1 L₀, approximately 145.35 Gyr. That output is a consequence of chosen inventory and power, not a prediction that a corresponding real star survives that long.

Test the zero-fuel boundary

Set the available region to zero. Every positive luminosity option now has zero possible completions, energy and support duration. The proposed power and its required reaction rate are not achieved output. Do not interpret a positive demand label as evidence that a fuel-free system is shining through this mechanism.

Transfer: diagnose a lifetime claim

A report finds the same budget duration for two selected cases and concludes that both stars have the same remaining main-sequence lifetime. Give the valid numerical conclusion and identify two missing physical ingredients before opening the worked response.

Check the fusion-budget transfer

The ratios of assumed deposited inventory to prescribed average photon power are equal. Actual remaining lifetime would require evidence about accessible remaining hydrogen, mixing and evolving luminosity, together with a stellar-structure/evolution model. Other reactions and energy storage may matter. The public calculation establishes a conditional fuel budget, not age or independent mastery.

Apply

Doubling both accessible fuel and prescribed photon power makes the conditional support duration:

Public practice checks a specific claim. It does not establish independent mastery.

Identify missing mixing and luminosity-history evidence before making an age claim.

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

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