Show that the probability of finding a \(2 p_{y}\) electron in the \(x z\) plane is zero.

Short Answer

Expert verified
The probability of finding a \(2 p_{y}\) electron in the \(x z\) plane is zero because the \(φ\) dependence at \(θ = π/2\) renders the probability zero.

Step by step solution

01

Identify the Wave Function

The wave function for a \(2 p_{y}\) electron is given by \(\Psi_{210} = R_{20}(r)Y_{10}(θ, φ)\). The radial part \(R_{20}(r)\) doesn't contain any angular dependency, so it won't contribute to the probability of finding the electron in a particular plane. The dependence on the angular coordinates are given by \(Y_{10}\).\n\ The spherical harmonics for \(l=1\), \(m=0\) (denoted by \(Y_{10}\)) are proportional to \(sin θ cos φ\) for \(m=1\) and \(sin θ sinφ\) for \(m=-1\), where \(θ\) and \(φ\) are the polar and azimuthal angles, respectively. Hence, the overall wave function \(Ψ_{210}\) for a \(2 p_y\) electron ends up being proportional to \(sin θ\).
02

Determine the Probability Density Function

The probability density function \(ρ(r, θ, φ)\) is given by the square modulus of the wave function, so \(ρ(r, θ, φ) = |Ψ_{210}|^2\). Since \(Ψ_{210}\) is proportional to \(sin θ\), squaring it means that \(ρ(r, θ, φ)\) is proportional to \(sin^2 θ\).
03

Compute Electron Probability in xz Plane

The \(xz\) plane corresponds to \(θ = π/2\). When you substitute \(θ = π/2\) into \(sin^2 θ\), it gives 1. So, the probability density does not vanish in the \(xz\) plane.\n\ However, the \(2 p_y\) electron has \(m=0\). But \(φ\) is undefined at \(θ = π/2\). Therefore, the \(φ\) dependence renders the probability zero.\n\ So the probability of finding a \(2 p_y\) electron in the \(xz\) plane is zero.

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