Controlled Thermonuclear Fusion — Question 2

Section 43-7 · Physics pages 7274–7275

Question 2 Alpha self-heating gives an idealized density-confinement requirement For equal D and T densities with total ion density n, use thermal energy density w = 3nkT, fusion rate density R = n2K/4, and alpha energy Eα = 3500 keV. Define loss density as w/τE. Let kT=10.0 keV and supplied reactivity K = 10−22 m3/s. Assume full alpha deposition. fusion α heat Schematic; labels, not drawing lengths, specify the data. (a) Derive the ideal Lawson self-heating condition on nτE without external heating. (b) Evaluate the bound and find the minimum confinement time at n = 1020 m−3.
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Question 2 - Solution Alpha self-heating gives an idealized density-confinement requirement fusion α heat (a) Method and calculation Pα/V = n2K 4 Eα ≥3nkT τE . nτE ≥12kT KEα . (b) Interpretation and further calculation nτE ≥ 12(10) 10−22(3500) = 3.42857 × 1020 m−3s . τE ≥3.42857 s (n = 1020 m−3). Physical check All losses are included in the defined energy-confinement time. This supplied fixed-temperature model omits impurities, incomplete alpha deposition and profile effects.

Question 2

Alpha self-heating gives an idealized density-confinement requirement

For equal D and T densities with total ion density n, use thermal energy density w=3nkTw=3nkT, fusion rate density R=n2K/4R=n^2K/4, and alpha energy Eα=3500E_\alpha=3500 keV. Define loss density as w/τEw/\tau_E. Let kT=10.0 keV and supplied reactivity K=10−22m3/sK=10^{-22}\,\mathrm{m^3/s}. Assume full alpha deposition.

Diagram shown in the original SVG worksheet.

  1. Derive the ideal Lawson self-heating condition on nτEn\tau_E without external heating.

  2. Evaluate the bound and find the minimum confinement time at n=1020m−3n=10^{20}\,\mathrm{m^{-3}}.

Question 2 - Solution

Alpha self-heating gives an idealized density-confinement requirement

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Pα/V=n2K4Eα≥3nkTτE.P_\alpha/V=\frac{n^2K}{4}E_\alpha\ge\frac{3nkT}{\tau_E}.nτE≥12kTKEα.\boxed{n\tau_E\ge\frac{12kT}{KE_\alpha}}.

(b) Interpretation and further calculation

nτE≥12(10)10−22(3500)=3.42857×1020m−3s.\boxed{n\tau_E\ge\frac{12(10)}{10^{-22}(3500)}=3.42857\times10^{20}\,\mathrm{m^{-3}s}}.τE≥3.42857s(n=1020m−3).\boxed{\tau_E\ge3.42857\,\mathrm s}\quad(n=10^{20}\,\mathrm{m^{-3}}).

Physical check

All losses are included in the defined energy-confinement time. This supplied fixed-temperature model omits impurities, incomplete alpha deposition and profile effects.