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Question: For a certain orbital $\Psi(r) = \frac{1}{16\sqrt{4}a_0^{3/2}}(1-\sigma)(\sigma^2 - 8\sigma + 12)e^{...

For a certain orbital Ψ(r)=1164a03/2(1σ)(σ28σ+12)eσ/2,σ=2rna0{a0=constant}\Psi(r) = \frac{1}{16\sqrt{4}a_0^{3/2}}(1-\sigma)(\sigma^2 - 8\sigma + 12)e^{-\sigma/2}, \sigma = \frac{2r}{na_0}\{a_0 = constant\}

The distance of nearest radial node from nucleus is xa0xa_0 while farthest radial node from nucleus is ya0ya_0.

Find (yx)(\frac{y}{x}).

Answer

6

Explanation

Solution

The radial nodes of an atomic orbital occur at distances from the nucleus where the radial part of the wave function is zero, excluding r=0r=0 and rr \to \infty.

The given wave function is Ψ(r)=1164a03/2(1σ)(σ28σ+12)eσ/2\Psi(r) = \frac{1}{16\sqrt{4}a_0^{3/2}}(1-\sigma)(\sigma^2 - 8\sigma + 12)e^{-\sigma/2}, where σ=2rna0\sigma = \frac{2r}{na_0}.

The radial part of the wave function is proportional to (1σ)(σ28σ+12)eσ/2(1-\sigma)(\sigma^2 - 8\sigma + 12)e^{-\sigma/2}.

The exponential term eσ/2=er/na0e^{-\sigma/2} = e^{-r/na_0} is never zero for finite rr, so the radial nodes are determined by the polynomial part: (1σ)(σ28σ+12)=0(1-\sigma)(\sigma^2 - 8\sigma + 12) = 0.

This equation is satisfied if either (1σ)=0(1-\sigma) = 0 or (σ28σ+12)=0(\sigma^2 - 8\sigma + 12) = 0.

Case 1: 1σ=0    σ=11-\sigma = 0 \implies \sigma = 1.

Case 2: σ28σ+12=0\sigma^2 - 8\sigma + 12 = 0. This is a quadratic equation. We can factor it or use the quadratic formula. We look for two numbers that multiply to 12 and add up to -8. These numbers are -2 and -6. So, the equation can be factored as (σ2)(σ6)=0(\sigma - 2)(\sigma - 6) = 0. This gives σ=2\sigma = 2 or σ=6\sigma = 6.

The values of σ\sigma for which the radial wave function is zero are σ=1,2,6\sigma = 1, 2, 6. These correspond to the radial nodes.

We are given the relation σ=2rna0\sigma = \frac{2r}{na_0}. We can use this to find the distances rr corresponding to these σ\sigma values: r=na0σ2r = \frac{na_0 \sigma}{2}.

For σ=1\sigma = 1, the distance is r1=na012=na02r_1 = \frac{na_0 \cdot 1}{2} = \frac{na_0}{2}. For σ=2\sigma = 2, the distance is r2=na022=na0r_2 = \frac{na_0 \cdot 2}{2} = na_0. For σ=6\sigma = 6, the distance is r3=na062=3na0r_3 = \frac{na_0 \cdot 6}{2} = 3na_0.

The distances of the radial nodes from the nucleus are na02\frac{na_0}{2}, na0na_0, and 3na03na_0. The nearest radial node is at the minimum of these distances, which is na02\frac{na_0}{2}. The farthest radial node is at the maximum of these distances, which is 3na03na_0.

We are given that the distance of the nearest radial node from the nucleus is xa0xa_0. So, xa0=na02xa_0 = \frac{na_0}{2}. This implies x=n2x = \frac{n}{2}.

We are given that the distance of the farthest radial node from the nucleus is ya0ya_0. So, ya0=3na0ya_0 = 3na_0. This implies y=3ny = 3n.

We need to find the ratio yx\frac{y}{x}. yx=3nn/2=3n2n=6\frac{y}{x} = \frac{3n}{n/2} = \frac{3n \cdot 2}{n} = 6.

The value of nn cancels out in the ratio.

The final answer is 6\boxed{6}.