GIVE ANSWER WITH EXPLANATION at the end of each step and final answer at the end~ PartD
Suppose NO binds to a surface with the oxygen immobilized on the protein surface leaving the nitrogen atom is free to continue a vibrational
motion. Assuming the NO bond spring constant remains unchanged, calculate the vibrational temperture for ¥N'60 bound to the surface at
T=300K. Hint: Calculate the reduced masses of free NO and NO bound with the O immobilized.
Elo -
Buis,surace= | Value Units
v PartE
Calculate the change in the molar vibrational internal energy when NO binds to the surface at T=300K.
EB os"
AUw= | Value Units
wv PartF
Calculate the change in the molar vibrational heat capacity when NO binds to a surface at T=300K.
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Question:
GIVE ANSWER WITH EXPLANATION at the end of each step and final answer at the end~ PartD
Suppose NO binds to a surface with the oxygen immobilized on the protein surface leaving the nitrogen atom is free to continue a vibrational
motion. Assuming the NO bond spring constant remains unchanged, calculate the vibrational temperture for ¥N'60 bound to the surface at
T=300K. Hint: Calculate the reduced masses of free NO and NO bound with the O immobilized.
Elo -
Buis,surace= | Value Units
v PartE
Calculate the change in the molar vibrational internal energy when NO binds to the surface at T=300K.
EB os"
AUw= | Value Units
wv PartF
Calculate the change in the molar vibrational heat capacity when NO binds to a surface at T=300K.
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This is AI generated Response.
Asked by: amu
Created at: 2025-07-27 04:35:22
Final Answer:
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Let's go step-by-step through each part.
---
### **Part D:**
**Calculate the vibrational temperature for \( ^{14}N^{16}O \) bound to the surface at \( T=300K \) (with O immobilized).**
#### **Step 1: Reduced Mass Calculation**
- **For free NO:**
Reduced mass,
\[
\mu_{\text{free}} = \frac{m_N m_O}{m_N + m_O}
\]
where \( m_N = 14 \) u, \( m_O = 16 \) u.
\[
\mu_{\text{free}} = \frac{14 \times 16}{14+16} = \frac{224}{30} = 7.47 \text{ u}
\]
- **For NO with O immobilized:**
Reduced mass (since O is fixed, only N moves):
\[
\mu_{\text{surface}} = m_N = 14 \text{ u}
\]
#### **Step 2: Vibrational Temperature (\( \theta_{\text{vib}} \))**
The vibrational temperature is:
\[
\theta_{\text{vib}} = \frac{h\nu}{k_B}
\]
And,
\[
\nu = \frac{1}{2\pi} \sqrt{\frac{k}{\mu}}
\]
Since spring constant \( k \) is unchanged, the ratio of vibrational temperatures is:
\[
\frac{\theta_{\text{vib,surface}}}{\theta_{\text{vib,free}}} = \sqrt{\frac{\mu_{\text{free}}}{\mu_{\text{surface}}}}
\]
\[
\theta_{\text{vib,surface}} = \theta_{\text{vib,free}} \sqrt{\frac{\mu_{\text{free}}}{\mu_{\text{surface}}}}
\]
- For NO, \( \theta_{\text{vib,free}} \approx 2740 \) K (you can look this up in a constants table).
\[
\theta_{\text{vib,surface}} = 2740 \times \sqrt{\frac{7.47}{14}}
\]
\[
\sqrt{\frac{7.47}{14}} = \sqrt{0.534} = 0.731
\]
\[
\theta_{\text{vib,surface}} = 2740 \times 0.731 \approx 2002 \text{ K}
\]
**Explanation:**
We first found the new reduced mass (since O is immobilized, only N vibrates). Then, knowing vibrational temperature depends inversely on the square root of reduced mass, we scaled the standard value for free NO by the ratio of reduced masses.
**Final Answer (Part D):**
\[
\boxed{2002 \ \text{K}}
\]
---
### **Part E:**
**Calculate the change in the molar vibrational internal energy when NO binds to the surface at T=300K.**
- Vibrational energy per mole:
\[
U_{\text{vib}} = R \frac{\theta_{\text{vib}}}{e^{\theta_{\text{vib}}/T}-1}
\]
So,
\[
\Delta U_{\text{vib}} = U_{\text{vib,surface}} - U_{\text{vib,free}}
\]
Let's calculate:
#### For free NO:
\[
U_{\text{vib,free}} = R \frac{2740}{e^{2740/300}-1}
\]
\[
\frac{2740}{300} = 9.13
\]
\[
e^{9.13} \approx 9233
\]
\[
U_{\text{vib,free}} = 8.314 \times \frac{2740}{9233-1} = 8.314 \times \frac{2740}{9232} = 8.314 \times 0.2966 = 2.465 \text{ J/mol}
\]
#### For surface-bound NO:
\[
U_{\text{vib,surface}} = R \frac{2002}{e^{2002/300}-1}
\]
\[
\frac{2002}{300} = 6.673
\]
\[
e^{6.673} \approx 790.6
\]
\[
U_{\text{vib,surface}} = 8.314 \times \frac{2002}{790.6-1} = 8.314 \times \frac{2002}{789.6} = 8.314 \times 2.536 = 21.10 \text{ J/mol}
\]
#### **Change:**
\[
\Delta U_{\text{vib}} = 21.10 - 2.465 = 18.64 \text{ J/mol}
\]
**Explanation:**
We used the formula for vibrational energy, plugged in the vibrational temperatures for both free and surface-bound NO, and subtracted to find the change.
**Final Answer (Part E):**
\[
\boxed{18.6 \ \text{J/mol}}
\]
---
### **Part F:**
**Calculate the change in the molar vibrational heat capacity at T=300 K.**
- Vibrational heat capacity,
\[
C_{V,\text{vib}} = R \left( \frac{\theta_{\text{vib}}}{T} \right)^2 \frac{e^{\theta_{\text{vib}}/T}}{(e^{\theta_{\text{vib}}/T} - 1)^2}
\]
#### For free NO:
\[
\left( \frac{2740}{300} \right)^2 \frac{e^{9.13}}{(e^{9.13}-1)^2}
\]
\[
(9.13)^2 = 83.39
\]
\[
\frac{e^{9.13}}{(e^{9.13}-1)^2} = \frac{9233}{(9232)^2} = \frac{9233}{85230824} = 1.08 \times 10^{-4}
\]
\[
C_{V,\text{vib,free}} = 8.314 \times 83.39 \times 1.08 \times 10^{-4} = 8.314 \times 0.00901 = 0.0749 \text{ J/mol K}
\]
#### For surface-bound NO:
\[
\left( \frac{2002}{300} \right)^2 \frac{e^{6.673}}{(e^{6.673}-1)^2}
\]
\[
(6.673)^2 = 44.53
\]
\[
\frac{e^{6.673}}{(e^{6.673}-1)^2} = \frac{790.6}{(789.6)^2} = \frac{790.6}{623507} = 0.001268
\]
\[
C_{V,\text{vib,surface}} = 8.314 \times 44.53 \times 0.001268 = 8.314 \times 0.0565 = 0.470 \text{ J/mol K}
\]
#### **Change:**
\[
\Delta C_{V,\text{vib}} = 0.470 - 0.0749 = 0.395 \text{ J/mol K}
\]
**Explanation:**
We calculated the vibrational heat capacity for both free and surface-bound NO, then subtracted to find the change.
**Final Answer (Part F):**
\[
\boxed{0.40 \ \text{J/mol K}}
\]
---
## **Summary of Final Answers:**
- **Part D:** \( \boxed{2002 \ \text{K}} \)
- **Part E:** \( \boxed{18.6 \ \text{J/mol}} \)
- **Part F:** \( \boxed{0.40 \ \text{J/mol K}} \)
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