Most probable value of r in ground state of hydrogen

In summary, the most probable value of r for the ground state of hydrogen is the Bohr radius (r_0), which corresponds to the peak of the probability density function P_{1s}(r). This value is obtained by setting the derivative of P_{1s}(r) equal to zero and solving for r.
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yxgao
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What is the most probable value of r for the grounds tate of hydrogen, and why? Is it just the Bohr radius?
 
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  • #2
Yes, it is the Bohr radius (which I'll call 'a'). The ground state wavefunction is:

ψ1s(r)=(1/π1/2a3/2)e-r/a.

The probability density is |ψ1s(r)|2, which is:

ρ1s(r)=|ψ1s(r)|2=(1/πa3)e-2r/a.

But that function is not going to give you the most probable radius. You have to take into account the fact that ρ1s is in spherical coordinates, whose volume element is:

dV=r2sin(φ)dr dθ dφ.

So, when you integrate ρ1s over all space, it gets multiplied by r2. Furthermore, since ψ1s is spherically symmetric, you can integrate over θ and φ to get what is called the radial probability density P1s(r):

P1s(r)=(4/a3)r2e-2r/a.

If you optimize this function, you will find that it has a relative maximum at r=a, the Bohr radius.
 
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  • #3
Thank you so much! That was very helpful!
 
  • #4
Particle Probability...


Quantum Hydrogen

Hydrogen wave function:
[tex]\psi_{1s} = \frac{1}{\sqrt{\pi r_0^3}} e^{-r/r_0}[/tex]

Bohr radius:
[tex]r_0 = \frac{\hbar}{\alpha M_e c}[/tex]

Probability density:
[tex]|\psi_{1s}|^2 = \left( \frac{1}{\pi r_0^3} \right) e^{-2r/r_0}[/tex]

[tex]P(r)dr = |\psi|^2 dV[/tex]

[tex]dV = 4 \pi r^2 dr[/tex]

[tex]P(r)dr = |\psi|^2 4 \pi r^2 dr[/tex]

Beta cloud probability:
[tex]P(r) = 4 \pi r^2 |\psi|^2[/tex]

Hydrogen probability density function:
[tex]P_{1s}(r) = \left( \frac{4r^2}{r_0^3} \right) e^{-2r/r_0}[/tex]

The most probable value of [tex]r[/tex] corresponds to the peak of the plot of [tex]P(r)[/tex] versus [tex]r[/tex]. The slope of the curve at this point is zero. To evaluate the most probable value of [tex]r[/tex] is by setting [tex]dP/dr = 0[/tex] and solving for [tex]r[/tex]:

[tex]\frac{dP}{dr} = 0[/tex]

[tex]\frac{dP}{dr} = \frac{d}{dr} \left[ \left( \frac{4r^2}{r_0^3} \right) e^{-2r/r_0} \right] = 0[/tex]

Derivative operation and simplification:
[tex]e^{-2r/r_0} \frac{d}{dr} (r^2) + r^2 \frac{d}{dr} (e^{-2r/r_0}) = 0[/tex]

[tex]2re^{-2r/r_0} + r^2(-2/r_0)e^{-2r/r_0} = 0[/tex]

[tex]2re^{-2r/r_0} - (2r^2/r_0)e^{-2r/r_0} = 0[/tex]

[tex]2r[1 - (r/r_0)]e^{-2r/r_0} = 0[/tex]

Expression satisfied if:
[tex]1 - \frac{r}{r_0} = 0[/tex]

Therefore:
[tex]\boxed{r = r_0}[/tex]

 
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1. What is the most probable value of r in the ground state of hydrogen?

The most probable value of r in the ground state of hydrogen is approximately 0.529 angstroms (0.053 nanometers).

2. How is the most probable value of r determined in the ground state of hydrogen?

The most probable value of r is determined by solving the Schrödinger equation for the hydrogen atom, which describes the wave function of the electron in the ground state.

3. Why is the most probable value of r important in the ground state of hydrogen?

The most probable value of r is important because it represents the most likely distance between the electron and nucleus in the ground state of hydrogen, and provides insight into the atom's stability and energy levels.

4. Is the most probable value of r the same for all hydrogen atoms in the ground state?

Yes, the most probable value of r is the same for all hydrogen atoms in the ground state because it is determined by the fundamental properties of the atom, such as the mass of the electron and the charge of the nucleus.

5. Can the most probable value of r change in excited states of hydrogen?

Yes, the most probable value of r can change in excited states of hydrogen as the electron's energy level increases, causing the atom to have a larger or smaller radius.

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