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What is the minimum uncertainty in the position of a \(0.50-\mathrm{kg}\) ball that is known to have a speed uncertainty of \(3.0 \times 10^{-28} \mathrm{~m} / \mathrm{s} ?\)

Short Answer

Expert verified
The minimum uncertainty in the ball's position is approximately \( 3.52 \times 10^{-7} \) meters.

Step by step solution

01

Understand the Heisenberg Uncertainty Principle

The Heisenberg Uncertainty Principle posits that there is an inherent limit to the precision with which the position and momentum of a particle can be simultaneously known. The principle is mathematically represented as \( \Delta x \cdot \Delta p \geq \frac{\hbar}{2} \), where \( \Delta x \) is the uncertainty in position, \( \Delta p \) is the uncertainty in momentum, and \( \hbar \) is the reduced Planck's constant, \( \hbar = 1.0545718 \times 10^{-34}\; \text{J}\cdot\text{s} \).
02

Calculate the Uncertainty in Momentum

The uncertainty in momentum \( \Delta p \) is given by \( \Delta p = m \cdot \Delta v \), where \( m \) is the mass of the ball and \( \Delta v \) is the uncertainty in its velocity. For this problem, \( m = 0.50\, \mathrm{kg} \) and \( \Delta v = 3.0 \times 10^{-28}\, \mathrm{m/s} \). Thus, \( \Delta p = 0.50 \cdot 3.0 \times 10^{-28} = 1.5 \times 10^{-28}\, \mathrm{kg}\cdot\mathrm{m/s} \).
03

Rearrange the Uncertainty Principle for Position

Rearrange the Heisenberg Uncertainty Principle formula to solve for \( \Delta x \):\[ \Delta x \geq \frac{\hbar}{2 \cdot \Delta p} \]
04

Plug In Known Values

We can now substitute the known values into the rearranged equation: \( \Delta x \geq \frac{1.0545718 \times 10^{-34}}{2 \cdot 1.5 \times 10^{-28}} \). Calculating this gives \( \Delta x \geq 3.515239333 \times 10^{-7}\, \mathrm{m} \).
05

Interpret Result

The minimum uncertainty in the position of the ball given the uncertainty in its speed is therefore approximately \( 3.52 \times 10^{-7} \) meters.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Quantum Mechanics
Quantum mechanics is a branch of physics that studies the behavior of matter and energy on very small scales, such as that of atoms and subatomic particles. This field revolutionized our understanding of the physical universe by revealing that, on these tiny scales, particles behave in ways that defy our classical intuitions.
One of the pivotal concepts in quantum mechanics is wave-particle duality. It suggests that every particle or quantum entity, such as electrons and photons, exhibits both wave-like and particle-like properties. This duality is not something that can be easily visualized in the classical sense, but it's a fundamental aspect of how particles of matter and light interact.
  • Wave-particle duality: Particles exhibit properties of both particles and waves.
  • Superposition: A quantum system can exist in multiple states at once.
  • Entanglement: Particles can become intertwined, with the state of one affecting the other, even over long distances.
These principles, among others, form the backbone of quantum theory and underpin phenomena like quantum tunneling, and the famous Schrödinger's cat thought experiment, which illustrates the concept of superposition.
Position Uncertainty
In quantum mechanics, the concept of position uncertainty refers to the idea that there is a fundamental limit to how precisely we can measure the position of a particle. This is one half of the famous Heisenberg Uncertainty Principle, which states that certain pairs of physical properties, like position and momentum, cannot both be known to arbitrarily high precision.
The Heisenberg Uncertainty Principle is often expressed as: \[ \Delta x \cdot \Delta p \geq \frac{\hbar}{2} \]where \( \Delta x \) is the uncertainty in position, \( \Delta p \) is the uncertainty in momentum, and \( \hbar \) is the reduced Planck's constant.
This principle implies that if you try to measure a particle's position more accurately, you will introduce greater uncertainty in its momentum measurement, and vice-versa. Thus, precise, simultaneous measurements of both cannot be achieved. It represents one of the key features that distinguish quantum mechanics from classical mechanics, where such limitations do not exist.
Momentum Uncertainty
Momentum uncertainty is the counterpart to position uncertainty in the Heisenberg Uncertainty Principle. It relates to how precisely we can determine the momentum of a particle. Momentum itself is defined as the product of a particle's mass and velocity:
\[ p = m \cdot v \] When we talk about momentum uncertainty, \( \Delta p \), it reflects the inevitable trade-off between precisely measuring a particle's momentum and its position. Reducing the uncertainty in one results in increased uncertainty in the other.
  • Increase in position precision âž” Increase in momentum uncertainty
  • Increase in momentum precision âž” Increase in position uncertainty
This uncertainty is not due to any flaw in measurement instruments but arises from the fundamental nature of particles as described by quantum mechanics. The relationship between position and momentum uncertainty is what gives rise to many intriguing quantum behaviors.
Reduced Planck's Constant
Reduced Planck's constant, represented by \( \hbar \), plays a crucial role in quantum mechanics, especially in the context of the Heisenberg Uncertainty Principle. It provides the scale at which quantum effects become significant.
The reduced Planck's constant is defined as:\[ \hbar = \frac{h}{2\pi} \] where \( h \) is Planck's constant, approximately \( 6.62607015 \times 10^{-34} \) joule seconds. The value of \( \hbar \) is about \( 1.0545718 \times 10^{-34} \) joule seconds.
This constant is foundational in quantum physics, indicating how the action is quantized. It sets the stage for quantum events and interactions by defining the limit to which classical notions of physics, like continuous measurements of position and momentum, start to falter. Hence, it is pivotal in calculations involving quantum systems, underlining the discrete and probabilistic nature of the microscopic world.

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Most popular questions from this chapter

Using a typical nuclear diameter of \(4.25 \times 10^{-15} \mathrm{~m}\) as its location uncertainty, compute the uncertainty in momentum and kinetic energy associated with an electron if it were part of the nucleus. For energies greater than a few \(\mathrm{MeV}\), particles such as electrons would escape the nucleus. What does this tell you about the likelihood that an electron resides in the nucleus of an atom?

Electrons are accelerated from rest through an electric potential difference. (a) If this potential difference increases to four times the original value, the new de Broglie wavelength will be (1) four times, (2) twice, (3) one-fourth, (4) one-half that of the original. Why? (b) If the original potential is \(250 \mathrm{kV}\) and the new potential is \(600 \mathrm{kV}\), what is the ratio of the new de Broglie wavelength to the original?

The lifetime of the excited state involved in a He-Ne laser of wavelength \(832.8 \mathrm{nm}\) is about \(10^{-4} \mathrm{~s}\). What is the ratio of the frequency width of a spectral line due to natural broadening to the frequency of the laser?

According to the Bohr theory of the hydrogen atom, the speed of the electron in the first Bohr orbit is \(2.19 \times 10^{6} \mathrm{~m} / \mathrm{s} .\) (a) What is the wavelength of the matter wave associated with the electron? (b) How does this wavelength compare with the circumference of the first Bohr orbit?

If the de Broglie wavelength associated with an electron is \(7.50 \times 10^{-7} \mathrm{~m},\) what is the electron's speed?

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