Give step-by-step solution with explanation and final answer:1. (24 Points) A particle of mass m is confined t0 a two-dimensional infinite potential well
Ged by he olin ory condos U3) =D for 01 3d 0 27 %
Sand Ue) = ouside hs res.
A. Using Schrodinger's equation, derive a formula for the energy states of the
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B. Identify the quantum numbers, energies, and degeneracy of the first two.
dene ery snes tev eg okies of Bg = £25
Question:
Give step-by-step solution with explanation and final answer:1. (24 Points) A particle of mass m is confined t0 a two-dimensional infinite potential well
Ged by he olin ory condos U3) =D for 01 3d 0 27 %
Sand Ue) = ouside hs res.
A. Using Schrodinger's equation, derive a formula for the energy states of the
eri
B. Identify the quantum numbers, energies, and degeneracy of the first two.
dene ery snes tev eg okies of Bg = £25
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**QUESTION RECAP:**
A particle of mass \( m \) is confined to a two-dimensional infinite potential well defined by:
- \( U(x, y) = 0 \) for \( 0 \leq x \leq 3L \) and \( 0 \leq y \leq 9L \)
- \( U(x, y) = \infty \) otherwise
**A. Using Schrödinger’s equation, derive a formula for the energy states of the particle.**
### **Step 1: Schrödinger Equation for 2D Infinite Well**
The time-independent Schrödinger equation is:
\[
-\frac{\hbar^2}{2m} \left( \frac{\partial^2 \Psi}{\partial x^2} + \frac{\partial^2 \Psi}{\partial y^2} \right) = E \Psi
\]
### **Step 2: Boundary Conditions**
- \( \Psi(0, y) = \Psi(3L, y) = 0 \)
- \( \Psi(x, 0) = \Psi(x, 9L) = 0 \)
### **Step 3: Separation of Variables**
Assume \( \Psi(x, y) = X(x)Y(y) \):
\[
-\frac{\hbar^2}{2m}\left( \frac{1}{X}\frac{d^2X}{dx^2} + \frac{1}{Y}\frac{d^2Y}{dy^2} \right) = E
\]
Let \( E = E_x + E_y \).
#### For \( x \):
\[
\frac{d^2X}{dx^2} + k_x^2 X = 0
\]
with boundary conditions \( X(0) = X(3L) = 0 \).
Solution: \( X(x) = \sin\left(\frac{n_x \pi x}{3L}\right) \), where \( n_x = 1, 2, 3, \ldots \)
So, \( k_x = \frac{n_x \pi}{3L} \)
#### For \( y \):
\[
\frac{d^2Y}{dy^2} + k_y^2 Y = 0
\]
with boundary conditions \( Y(0) = Y(9L) = 0 \).
Solution: \( Y(y) = \sin\left(\frac{n_y \pi y}{9L}\right) \), where \( n_y = 1, 2, 3, \ldots \)
So, \( k_y = \frac{n_y \pi}{9L} \)
### **Step 4: Energy Formula**
\[
E_{n_x, n_y} = \frac{\hbar^2}{2m} \left( k_x^2 + k_y^2 \right)
= \frac{\hbar^2}{2m} \left[ \left( \frac{n_x \pi}{3L} \right)^2 + \left( \frac{n_y \pi}{9L} \right)^2 \right]
= \frac{\hbar^2 \pi^2}{2m L^2} \left( \frac{n_x^2}{9} + \frac{n_y^2}{81} \right)
\]
---
**B. Identify the quantum numbers, energies, and degeneracy of the first two degenerate energy states that are integer multiples of \( E_0 = \frac{\hbar^2 \pi^2}{2m L^2} \).**
### **Step 1: Express Energy in terms of \( E_0 \)**
\[
E_{n_x, n_y} = E_0 \left( \frac{n_x^2}{9} + \frac{n_y^2}{81} \right)
\]
We are to find the first two degenerate energy states (states with different quantum numbers but same energy), with energies that are integer multiples of \( E_0 \).
### **Step 2: Find Degenerate States**
Let’s try some integer values for \( n_x \) and \( n_y \):
#### **Try \( n_x = 3 \), \( n_y = 0 \) (but \( n_y \geq 1 \)), so try \( n_x = 3 \), \( n_y = 9 \):**
\[
E_{3,9} = E_0 \left( \frac{9}{9} + \frac{81}{81} \right) = E_0 (1+1) = 2 E_0
\]
#### **Try \( n_x = 6 \), \( n_y = 0 \) (not allowed), so try \( n_x = 6 \), \( n_y = 9 \):**
\[
E_{6,9} = E_0 \left( \frac{36}{9} + \frac{81}{81} \right) = E_0 (4 + 1) = 5 E_0
\]
#### **Try \( n_x = 9 \), \( n_y = 9 \):**
\[
E_{9,9} = E_0 \left( \frac{81}{9} + \frac{81}{81} \right) = E_0 (9 + 1) = 10 E_0
\]
#### **Try \( n_x = 6 \), \( n_y = 6\):**
\[
E_{6,6} = E_0 \left( \frac{36}{9} + \frac{36}{81} \right) = E_0 (4 + 0.444) = 4.444 E_0
\]
—not integer.
#### **Try \( n_x = 0 \), \( n_y = 9 \): Not allowed; both quantum numbers must be ≥1.**
#### **Try \( n_x = 9 \), \( n_y = 0 \): Not allowed.**
#### **Try \( n_x = 6 \), \( n_y = 6 \): Already checked.**
#### **Try \( n_x = 1 \), \( n_y = 9 \):**
\[
E_{1,9} = E_0 \left( \frac{1}{9} + \frac{81}{81} \right) = E_0 \left( \frac{1}{9} + 1 \right) = E_0 \left( \frac{10}{9} \right)
\]
—not integer.
#### **Try \( n_x = 3 \), \( n_y = 9 \):**
Already got \( 2 E_0 \).
#### **Try \( n_x = 6 \), \( n_y = 9 \):**
Already got \( 5 E_0 \).
#### **Try \( n_x = 9 \), \( n_y = 0 \), not allowed.**
#### **Try \( n_x = 3 \), \( n_y = 18 \):**
\[
E_{3,18} = E_0 \left( \frac{9}{9} + \frac{324}{81} \right) = E_0 (1 + 4) = 5 E_0
\]
Degenerate with \( (6,9) \).
#### **Try \( n_x = 6 \), \( n_y = 15 \):**
\[
E_{6,15} = E_0 \left( \frac{36}{9} + \frac{225}{81} \right) = E_0 (4 + 2.778) = 6.778 E_0
\]
—not integer.
### **Summarize:**
#### **First two degenerate integer-multiple states:**
1. \( E = 2E_0 \):
- \( (n_x, n_y) = (3, 9) \) and \( (9, 3) \) (But \( n_y \) must be ≤ 9, so only \( (3,9) \) valid in this well.)
- DEGENERACY: 1
2. \( E = 5E_0 \):
- \( (n_x, n_y) = (6,9) \) and \( (3,18) \) (but \( n_y \leq 9 \), so only \( (6,9) \) is valid)
- DEGENERACY: 1
#### **Degeneracy:**
In this well, due to the asymmetric boundaries, most states are non-degenerate (degeneracy 1), unless \( \frac{n_x^2}{9} = \frac{n_y^2}{81} \) and both quantum numbers are within allowed limits.
---
## **Final Answers**
### **A. Energy Formula**
\[
\boxed{
E_{n_x, n_y} = \frac{\hbar^2 \pi^2}{2m L^2} \left( \frac{n_x^2}{9} + \frac{n_y^2}{81} \right)
}
\]
where \( n_x = 1, 2, 3, \ldots \), \( n_y = 1, 2, 3, \ldots \)
### **B.**
- **First degenerate integer-multiple state:** \( E = 2E_0 \), quantum numbers \( (n_x, n_y) = (3,9) \); degeneracy = 1
- **Second degenerate integer-multiple state:** \( E = 5E_0 \), quantum numbers \( (n_x, n_y) = (6,9) \); degeneracy = 1
If you have further questions about the degeneracy or want to check more states, let me know!
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