The energy E in joule (J) associated with the temperature T in kelvin (K) is equal to kBT, where kB is the constant of Boltzmann [1,2]. Now, 1eV = (e/C) J, where e/C ≡ {e} is the absolute value of the charge of an electron in coulomb (C = A s = ampère × second). These bring one to [3]:
1 eV = 1.602 177 33 × 10-19 J = 11 604.45 K.
Thus, 1 eV is approximately equal to 104 K, or 1 K approximately equal to 10-4 eV.
Nityananda Das :My pleasure. As for your first question, the answer is in the positive (my last sentence in my previous comment on this page conveys the same thing).
Regarding your last question, temperature T is a thermodynamic parameter associated with a system in thermal equilibrium. Depending on which thermodynamic potential one uses, T may or may not be a thermodynamic variable. The internal energy E = E(S,V,N) of a system in thermal equilibrium (with S = entropy, V = volume, and N = number of particles) is not an explicit function of T; E only implicitly depends on T through the temperature dependence of S. In contrast, the Helmholtz free energy F = F(T,V,N) = E - TS is an explicit function of T. In short, temperature of a system in thermal equilibrium is not equal to its energy divided by the Boltzmann constant; a given amount of energy can however be expressed (as a matter of convenience) in terms of some effective temperature (which is to be distinguished from the T just discussed) in units of the Boltzmann constant.