(a) Use Laplace's method to obtain an approximation to , and state its fractional…

PHYSICS · Subjective · Fermi University Physics · Mathematical Methods for Physics · Plasma Physics · Fusion plasmas

The Nucleus Resolved, Ch Fusion: the cross section computed and the power balance made honest

Problem

(a) Use Laplace's method to obtain an approximation to 5!=∫0∞x5e−x dx5! = \int_0^\infty x^5e^{-x}\,\mathrm{d}x, and state its fractional error compared with the exact value 120120. Compare that error with the leading correction 1/(12n)1/(12n) at n=5n=5. (b) Starting from the plasma power balance dWdt=Pα+Pext−Pbrems−Pimp−WτE,\frac{\mathrm{d}W}{\mathrm{d}t} = P_\alpha + P_{\rm ext} - P_{\rm brems} - P_{\rm imp} - \frac{W}{\tau_E}, with thermal energy density W=3nkBTW = 3nk_BT and alpha heating Pα=14n2⟨σv⟩EαP_\alpha = \tfrac14 n^2\langle\sigma v\rangle E_\alpha for an equimolar deuterium-tritium plasma, derive the ignition condition nτE≥12kBT/(⟨σv⟩Eα)n\tau_E \ge 12k_BT/(\langle\sigma v\rangle E_\alpha) by setting Pext=Pbrems=Pimp=0P_{\rm ext} = P_{\rm brems} = P_{\rm imp} = 0 and dW/dt=0\mathrm{d}W/\mathrm{d}t = 0. (c) Evaluate the ignition value of nτEn\tau_E at kBT=20 keVk_BT = 20\,\mathrm{keV}, given ⟨σv⟩=4.2×10−22 m3 s−1\langle\sigma v\rangle = 4.2\times10^{-22}\,\mathrm{m^3\,s^{-1}} and Eα=3.5 MeVE_\alpha = 3.5\,\mathrm{MeV}.

Browse the problem library