Step 1: Concept Overview:
The problem requires evaluating an Assertion and a Reason concerning the statistical properties of electrons in a conductor at thermal equilibrium (without external fields).
Step 2: Detailed Analysis:
Assertion (A): The assertion states that, lacking an external field, the electron gas is in equilibrium and can be statistically described. It correctly identifies the Fermi-Dirac distribution for a degenerate electron gas (typical of metals) and the Maxwell-Boltzmann distribution for a non-degenerate gas (relevant for semiconductors under specific conditions or classical gases). This is a fundamental principle in statistical mechanics and solid-state physics. Therefore, Assertion (A) is true.
Reason (R): The reason describes the electron gas's equilibrium state. Without an electric field, electron motion is random. For each electron with velocity \(\vec{v}\), another exists with velocity \(-\vec{v}\). This equal distribution in opposite directions results in a zero average velocity and no net current. This symmetry (equal probability for \(+v_x\) and \(-v_x\)) implies a symmetric velocity distribution function. This accurately depicts the microscopic equilibrium. Therefore, Reason (R) is true.
Connection: Reason (R) explains {why} the system is in equilibrium. The symmetric velocity distribution, leading to zero average velocity, defines the equilibrium state described mathematically by the distribution functions in Assertion (A). The symmetric distribution and zero net flow are precisely what the equilibrium Fermi-Dirac function represents. Hence, (R) correctly explains (A).
Step 3: Conclusion:
Both Assertion (A) and Reason (R) are true, and Reason (R) correctly explains Assertion (A).