\( -27.2 \) eV
Step 1: Understanding energy levels of the hydrogen atom
The total energy of an electron in the \( n \)th energy level of a hydrogen atom is given by: \[ E_n = \frac{E_1}{n^2} \] where: - \( E_1 = -13.6 \) eV (ground state energy), - \( n \) is the principal quantum number. For the first excited state, \( n = 2 \): \[ E_2 = \frac{-13.6}{2^2} = \frac{-13.6}{4} = -3.4 \text{ eV} \] Step 2: Relationship between total energy and potential energy
The potential energy (\( U \)) in an atomic system is related to the total energy by: \[ U = 2E_n \] Substituting \( E_2 = -3.4 \) eV: \[ U = 2 \times (-3.4) \] \[ U = -6.8 \text{ eV} \] Thus, the potential energy of the electron in the first excited state is \( -6.8 \) eV.
Given the function:
\[ f(x) = \frac{2x - 3}{3x - 2} \]
and if \( f_n(x) = (f \circ f \circ \ldots \circ f)(x) \) is applied \( n \) times, find \( f_{32}(x) \).
For \( n \in \mathbb{N} \), the largest positive integer that divides \( 81^n + 20n - 1 \) is \( k \). If \( S \) is the sum of all positive divisors of \( k \), then find \( S - k \).
If the real-valued function
\[ f(x) = \sin^{-1}(x^2 - 1) - 3\log_3(3^x - 2) \]is not defined for all \( x \in (-\infty, a] \cup (b, \infty) \), then what is \( 3^a + b^2 \)?