give answer in 2 step with all parts explanation at the end of each step and final answer at the end: A thin solid barrier in the xy - plane has a 13.7um diameter circular hole. An elect with vx = 0.00m/s passes through the hole. Afterward, within what range is vx likely to be?
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give answer in 2 step with all parts explanation at the end of each step and final answer at the end: A thin solid barrier in the xy - plane has a 13.7um diameter circular hole. An elect with vx = 0.00m/s passes through the hole. Afterward, within what range is vx likely to be?
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Asked by: Rahul
Created at: 2025-11-27 05:15:59
Asked by: Rahul
Created at: 2025-11-27 05:15:59
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# Step 1: Apply the Uncertainty Principle
When an electron passes through a hole of diameter \( d = 13.7\,\mu\text{m} = 13.7 \times 10^{-6}\,\text{m} \), its position in the \( x \)-direction is known within about \( \Delta x \approx d \).
By Heisenberg’s uncertainty principle:
\[
\Delta x \, \Delta p_x \geq \frac{\hbar}{2}
\]
Given:
- \( \Delta x = 13.7 \times 10^{-6}\,\text{m} \)
- \( \hbar = 1.055 \times 10^{-34}\,\text{Js} \)
So,
\[
\Delta p_x \geq \frac{\hbar}{2 \Delta x}
\]
\[
\Delta p_x \geq \frac{1.055 \times 10^{-34}}{2 \times 13.7 \times 10^{-6}}
\]
\[
\Delta p_x \geq \frac{1.055 \times 10^{-34}}{2.74 \times 10^{-5}}
\]
\[
\Delta p_x \geq 3.85 \times 10^{-30}\,\text{kg m/s}
\]
**Explanation**:
- The width of the hole sets the uncertainty in position (\( \Delta x \)).
- The uncertainty principle gives us the minimum uncertainty in momentum (\( \Delta p_x \)).
---
# Step 2: Convert Momentum Uncertainty to Velocity Range
The electron's momentum in \( x \)-direction: \( p_x = m v_x \).
So,
\[
\Delta p_x = m \Delta v_x
\]
The mass of the electron \( m = 9.11 \times 10^{-31}\,\text{kg} \).
\[
\Delta v_x = \frac{\Delta p_x}{m}
\]
\[
\Delta v_x = \frac{3.85 \times 10^{-30}}{9.11 \times 10^{-31}}
\]
\[
\Delta v_x \approx 4.23\,\text{m/s}
\]
Because the electron initially had \( v_x = \), after passing through the hole, its \( v_x \) is likely in the range:
\[
-2.12\,\text{m/s} \leq v_x \leq +2.12\,\text{m/s}
\]
This range is \( \pm \Delta v_x/2 \), but commonly, the full uncertainty is taken as the range \( (-\Delta v_x/2, +\Delta v_x/2) \) or just \( \pm \Delta v_x \). Here, using the full calculated uncertainty as the likely spread:
\[
-4.23\,\text{m/s} \leq v_x \leq +4.23\,\text{m/s}
\]
**Explanation**:
- The range for \( v_x \) comes from the uncertainty in momentum, divided by the electron mass.
- After passing through the hole, the electron’s \( v_x \) could be positive or negative within this range.
---
# Final Answer
**After passing through the hole, the electron’s \( v_x \) is likely in the range:**
\[
-4.23\,\text{m/s} \leq v_x \leq +4.23\,\text{m/s}
\]
**This range is set by the uncertainty principle due to the position constraint of the hole.**
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