Start Learning Free

Before You Begin

Question #42861

Difficulty: 8/10 | 🟢 Free

The Question

An electron of mass mm is confined in a one-dimensional infinite potential well of width LL between x=0x = 0 and x=Lx = L. The electron is in its first excited state (n=2n=2). Let Δx\Delta x, Δp\Delta p, and ΔE\Delta E denote the standard deviations (uncertainties) in the position, momentum, and total energy of the electron in this state, respectively, and let hh be Planck's constant. A flawed argument suggests that because the probability density is exactly zero at the node x=L/2x = L/2, the electron is perfectly excluded from this point, implying a local spatial uncertainty Δx→0\Delta x \to 0 and thus ΔE→∞\Delta E \to \infty. By correctly applying the principles of quantum mechanics to the entire stationary state, determine the true values of Δx\Delta x, Δp\Delta p, and ΔE\Delta E.

Options

  • A.

    Δx=L112−18π2,  Δp=hL,  ΔE=0\Delta x = L\sqrt{\frac{1}{12} - \frac{1}{8\pi^2}}, \; \Delta p = \frac{h}{L}, \; \Delta E = 0

  • B.

    Δx=0,  Δp→∞,  ΔE→∞\Delta x = 0, \; \Delta p \to \infty, \; \Delta E \to \infty

  • C.

    Δx=L112−12π2,  Δp=h2L,  ΔE=3h28mL2\Delta x = L\sqrt{\frac{1}{12} - \frac{1}{2\pi^2}}, \; \Delta p = \frac{h}{2L}, \; \Delta E = \frac{3h^2}{8mL^2}

  • D.

    Δx=L112−18π2,  Δp=hL,  ΔE=h22mL2\Delta x = L\sqrt{\frac{1}{12} - \frac{1}{8\pi^2}}, \; \Delta p = \frac{h}{L}, \; \Delta E = \frac{h^2}{2mL^2}

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Standing Wave Nodes/Antinodes|Heisenberg's Limitation|Energy Level Scaling

Why This Question Is Tricky

Common Mistakes

This question tests the fundamental distinction between a mathematical node in a wavefunction and the physical localization of a particle.

Students often fall into the trap of assuming that because the probability density is zero at a node, the particle is 'perfectly excluded' from that exact point, leading them to incorrectly assign a local spatial uncertainty Δx→0\Delta x \to 0.

By misapplying Heisenberg's uncertainty principle to this single point, they deduce infinite momentum and energy uncertainties.

In reality, Heisenberg's principle applies to the standard deviations of the entire wave packet.

For a stationary state, the particle is delocalized across the entire potential well, yielding a finite Δx\Delta x and Δp\Delta p.

Furthermore, because it is an energy eigenstate, the energy is exactly defined, meaning ΔE=0\Delta E = 0, regardless of the spatial nodal structure.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterWaves - Class 11 Part 2
ConceptStanding Wave Nodes/Antinodes
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree