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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Ten percent at one nominal solar luminosity gives approximately 7.268 Gyr as a budget ratio.
Open the experimentPredict
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.
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.
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.
| Quantity | Selected demand | Same inventory, 1 nominal solar luminosity |
|---|---|---|
| Accessible region kg | 2.00000e+29 | 2.00000e+29 |
| Hydrogen inventory kg | 1.40000e+29 | 1.40000e+29 |
| Possible net completions | 2.09138e+55 | 2.09138e+55 |
| Helium product rest mass kg | 1.39003e+29 | 1.39003e+29 |
| Total released budget J | 8.95692e+43 | 8.95692e+43 |
| Neutrino budget J | 1.77591e+42 | 1.77591e+42 |
| Deposited budget J | 8.77933e+43 | 8.77933e+43 |
| Prescribed photon demand W | 3.82800e+26 | 3.82800e+26 |
| Required completions per second | 9.11894e+37 | 9.11894e+37 |
| Required hydrogen processing kg/s | 6.10434e+11 | 6.10434e+11 |
| Required rest-mass conversion kg/s | 4.34538e+9 | 4.34538e+9 |
| Implied neutrino power at required rate W | 7.74338e+24 | 7.74338e+24 |
| Conditional support duration Gyr | 7.26751 | 7.26751 |
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.
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Public practice checks a specific claim. It does not establish independent mastery.
Identify missing mixing and luminosity-history evidence before making an age claim.
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