To derive the correct Schrödinger wave equation for an electron with total energy \( E \) and potential energy \( V \), we can follow these steps:
### Step 1: Understand the Schrödinger Wave Equation
The Schrödinger wave equation is a fundamental equation in quantum mechanics that describes how the quantum state of a physical system changes over time. It is expressed in terms of the wave function \( \psi \).
### Step 2: Write the Time-Independent Schrödinger Equation
For a particle in a potential \( V \), the time-independent Schrödinger equation can be written as:
\[
-\frac{\hbar^2}{2m} \nabla^2 \psi + V \psi = E \psi
\]
where:
- \( \hbar \) is the reduced Planck's constant,
- \( m \) is the mass of the electron,
- \( \nabla^2 \) is the Laplacian operator, which in three dimensions is given by:
\[
\nabla^2 = \frac{\partial^2}{\partial x^2} + \frac{\partial^2}{\partial y^2} + \frac{\partial^2}{\partial z^2}
\]
### Step 3: Rearranging the Equation
Rearranging the equation gives:
\[
-\frac{\hbar^2}{2m} \nabla^2 \psi = (E - V) \psi
\]
### Step 4: Multiply by \(-\frac{2m}{\hbar^2}\)
To express the equation in a standard form, we can multiply both sides by \(-\frac{2m}{\hbar^2}\):
\[
\nabla^2 \psi + \frac{2m}{\hbar^2} (V - E) \psi = 0
\]
### Step 5: Substitute \( \hbar \) with \( h \)
Since \( \hbar = \frac{h}{2\pi} \), we can express the equation in terms of \( h \):
\[
\nabla^2 \psi + \frac{8\pi^2 m}{h^2} (V - E) \psi = 0
\]
### Step 6: Final Form of the Schrödinger Wave Equation
Thus, the final form of the Schrödinger wave equation for an electron with total energy \( E \) and potential energy \( V \) is:
\[
\nabla^2 \psi + \frac{8\pi^2 m}{h^2} (V - E) \psi = 0
\]
### Conclusion
The correct Schrödinger wave equation is:
\[
\frac{\partial^2 \psi}{\partial x^2} + \frac{\partial^2 \psi}{\partial y^2} + \frac{\partial^2 \psi}{\partial z^2} + \frac{8\pi^2 m}{h^2} (V - E) \psi = 0
\]
The correct option that expresses this equation is option C.
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