for the process `._1H^2+._1H^3to._2He^4+n+Q`
`Q=[m(._1H^2)+m(._1H^3)-m(._2He^4)-m_n]xx931MeV`.
`=(2.014102+3.016049-4.002603-1.00867)xx931MeV=0.018878xx931=17.58MeV`
(b) Repulsive potential energy of two nuclei when they almost touch eachother is
`=(q^2)/(4pi in_0(2r))=(9xx10^9(1.6xx10^(-19))^2)/(2xx2xx10^(-15))"joule" =5.67xx10^(-14)"joule"`
Classicaly, K.E. at least equal to this amount is required to overcome Coulomb repulsion. Using the relation `K.E.=2xx3/2kT " " T=((K.E.))/(3k)=(5.76xx10^(-14))/(3xx1.38xx10^(-23))=1.39xx10^9K`
In actual practice, the temperature required for trigerring the reaction is somewhat less.