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What is the difference in energy ΔE between the n=0 and n=1 vibrational states for diatomic hydrogen? The effective force constant k for diatomic hydrogen is 576N/m .

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The energy difference (
\( \Delta E \)) between the n=0 and n=1 vibrational states for diatomic hydrogen is approximately
\(9.35 * 10^(-21) \, \text{J}\).

The energy difference (
\( \Delta E \)) between vibrational states in a diatomic molecule can be calculated using the formula for harmonic oscillator energy levels:


\[ \Delta E = h \cdot \\u \]

where:

- h is Planck's constant (
\(6.626 * 10^(-34) \, \text{J} \cdot \text{s}\)),

-
\( \\u \) is the vibrational frequency.

For a diatomic molecule, the vibrational frequency (
\( \\u \)) can be calculated using the formula:


\[ \\u = (1)/(2\pi) \sqrt{(k)/(\mu)} \]

where:

- k is the force constant,

-
\( \mu \) is the reduced mass of the system.

The reduced mass (
\( \mu \)) for a diatomic molecule can be calculated using:


\[ \mu = (m_1 \cdot m_2)/(m_1 + m_2) \]

where:

-
\( m_1 \) and \( m_2 \) are the masses of the two atoms.

For diatomic hydrogen (
\( H_2 \)), each hydrogen atom has a mass of approximately
\(1.0079 \, \text{u}\) (atomic mass units).

Now, let's plug in the values:


\[ \mu = \frac{(1.0079 \, \text{u})^2}{1.0079 \, \text{u} + 1.0079 \, \text{u}} \]


\[ \mu \approx 0.5039 \, \text{u} \]


\[ \\u = (1)/(2\pi) \sqrt{\frac{576 \, \text{N/m}}{0.5039 \, \text{u}}} \]


\[ \\u \approx 1.412 * 10^(13) \, \text{Hz} \]

Now, calculate
\( \Delta E \):


\[ \Delta E = h \cdot \\u \]


\[ \Delta E \approx (6.626 * 10^(-34) \, \text{J} \cdot \text{s}) \cdot (1.412 * 10^(13) \, \text{Hz}) \]


\[ \Delta E \approx 9.35 * 10^(-21) \, \text{J} \]

Therefore, the energy difference (
\( \Delta E \)) between the n=0 and n=1 vibrational states for diatomic hydrogen is approximately
\(9.35 * 10^(-21) \, \text{J}\).

User Vasyl Demin
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