Concept: Nodes in atomic orbitals
A {node} is a region in space where the probability of finding an electron is zero.
Mathematically, this occurs where the {wave function} \(\psi = 0\).
For hydrogen-like orbitals:
Radial nodes occur where the radial part of the wave function becomes zero.
The number of radial nodes is given by:
\[
n - l - 1
\]
Step 1: Identify nodes in the \(2s\) orbital
For the \(2s\) orbital:
\[
n = 2,\quad l = 0
\]
\[
\text{Number of radial nodes} = 2 - 0 - 1 = 1
\]
Thus, the \(2s\) orbital has one spherical nodal surface, as shown in Figure 1.
Step 2: Relation between probability density and wave function
Electron probability density is proportional to \(|\psi|^2\).
A nodal surface corresponds to \(\psi = 0\), not merely a minimum.
Hence, we must locate the point in Figure 2 where the wave function crosses the \(x\)-axis.
Step 3: Analyse Figure 2
From the graph of \(\psi_{2s}(x)\):
Point \(A\): \(\psi\) is positive and maximum.
Point \(B\): \(\psi = 0\) (crosses the axis).
Point \(C\): \(\psi\) is negative and minimum.
Point \(D\): \(\psi\) is negative but non-zero.
Only point \(B\) satisfies the condition:
\[
\psi_{2s} = 0
\]
Step 4: Connect Figure 1 and Figure 2
The spherical nodal surface in Figure 1 corresponds to a specific radius where:
\[
\psi_{2s}(r) = 0
\]
When represented along a single axis (Figure 2), this node appears as a zero-crossing of the wave function.
Final Answer:
\[
\boxed{\text{Point B}}
\]