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The Heisenberg uncertainty principle can be expressed in the form $$\Delta E \cdot \Delta t \geq \frac{h}{4 \pi}$$ where \(E\) represents energy and \(t\) represents time. Show that the units for this form are the same as the units for the form used in this chapter: $$\Delta x \cdot \Delta(m v) \geq \frac{h}{4 \pi}$$

Short Answer

Expert verified
In the given forms of the Heisenberg Uncertainty Principle, for the first form \(\Delta E \cdot \Delta t \geq \frac{h}{4 \pi}\), the units are Joule-seconds (J·s), while for the second form \(\Delta x \cdot \Delta(mv) \geq \frac{h}{4 \pi}\), the units can be converted into Joule-seconds as well (J·s). Therefore, the units for both forms are the same.

Step by step solution

01

Identify the units for each variable

First, we should determine the units for each variable in SI units: - \(E\): Energy, measured in Joules (J) - \(t\): Time, measured in seconds (s) - \(x\): Position, measured in meters (m) - \(m\): Mass, measured in kilograms (kg) - \(v\): Velocity, measured in meters per second (m/s) - \(h\): Planck's constant, measured in Joule-seconds (J·s)
02

Analyze the first form, \(\Delta E \cdot \Delta t \geq \frac{h}{4 \pi}\)

Now that we have determined the units for each variable, let's analyze the units for each term in the first form of Heisenberg Uncertainty Principle: $$\Delta E \cdot \Delta t \geq \frac{h}{4 \pi}$$ Substitute the SI units for the variables: $$\Delta(\text{J}) \cdot \Delta(\text{s}) \geq \frac{\text{J} \cdot \text{s}}{4 \pi}$$ Simplify: $$\text{J} \cdot \text{s} \geq \frac{\text{J} \cdot \text{s}}{4 \pi}$$
03

Analyze the second form, \(\Delta x \cdot \Delta(mv) \geq \frac{h}{4 \pi}\)

Now let's analyze the units for each term in the second form of Heisenberg Uncertainty Principle: $$\Delta x \cdot \Delta(mv) \geq \frac{h}{4 \pi}$$ Substitute the SI units for the variables: $$\Delta(\text{m}) \cdot \Delta(\text{kg} \cdot \frac{\text{m}}{\text{s}}) \geq \frac{\text{J} \cdot \text{s}}{4 \pi}$$ Simplify: $$\text{m} \cdot (\text{kg} \cdot \text{m}/\text{s}) \geq \frac{\text{J} \cdot \text{s}}{4 \pi}$$ Now, we need to convert the left-hand side of this inequality to Joule-seconds. Recall that the relationship between Joules, kilograms, and meters is given by the formula \(E = \frac{1}{2}mv^2\). So, we can substitute \(\text{J} = \text{kg} \cdot (\text{m}/\text{s})^2\): $$\text{m} \cdot (\text{kg} \cdot \text{m}/\text{s}) = \text{J} \cdot \text{s}$$
04

Compare the units of both forms

From steps 2 and 3, we have the following inequalities: Inequality 1: $$\text{J} \cdot \text{s} \geq \frac{\text{J} \cdot \text{s}}{4 \pi}$$ Inequality 2: $$\text{J} \cdot \text{s} \geq \frac{\text{J} \cdot \text{s}}{4 \pi}$$ It can be seen that the units on both sides of the inequalities in step 2 and 3 are the same, which means that both forms of the Heisenberg Uncertainty Principle have the same units and are consistent with each other.

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Key Concepts

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

Energy-Time Uncertainty
The energy-time uncertainty principle is a fundamental concept in quantum physics that suggests a limitation in measuring the precision of energy (E) and time (t) simultaneously. According to this principle, the uncertainty in energy (\(\Delta E\)) multiplied by the uncertainty in time (\(\Delta t\)) is never less than a specific minimum value, represented by Planck's constant divided by\(4 \pi\):
  • The formula is written as\(\Delta E \cdot \Delta t \geq \frac{h}{4 \pi}\).

This equation implies that if one measures energy with great precision (reducing\(\Delta E\)), this precision adversely impacts the ability to measure time accurately (increases\(\Delta t\)), and vice versa.

The significance of energy-time uncertainty lies in its connection to the lifetime of quantum states. For example, when subatomic particles exist briefly, their energy measurements naturally exhibit considerable uncertainty. This principle aligns with real-world observations, allowing phenomena such as imperfect energy conservation over extremely short durations.
Position-Momentum Uncertainty
The position-momentum uncertainty is perhaps the most well-known form of the Heisenberg Uncertainty Principle. It relates the uncertainties in measuring the position (\(x\)) and the momentum (\(p\)) of a particle simultaneously.
  • Mathematically, this is expressed as:\(\Delta x \cdot \Delta p \geq \frac{h}{4 \pi}\).

Momentum is defined as the product of a particle's mass (\(m\)) and velocity (\(v\)), i.e.,\(p = mv\). Therefore, the uncertainty in momentum,\(\Delta(mv)\), poses a practical limit on how precisely position and momentum can be simultaneously known.

The foundational insight of position-momentum uncertainty lies in its modern physical implications - it sets a boundary on the classical notion of localized particles with definite paths. This non-deterministic nature reveals why electrons do not crash into the nucleus of an atom; instead, they form stable orbitals dictated by probabilities rather than definitive trajectories.

This quantum uncertainty is essential for explaining phenomena such as wavefunction probabilistic behavior and forms the basis of quantum mechanics.
Unit Consistency in Physics
Unit consistency is crucial across all areas of physics and plays a key role in validating theoretical expressions.

For any physical equation to be valid, both sides must have consistent units. In the context of the Heisenberg Uncertainty Principle, checking for unit consistency helps us ensure that different expressions of the principle are equivalent.
  • For instance, in both the energy-time and position-momentum forms,the right-hand side \(\frac{h}{4 \pi} \)is expressed in Joule-seconds (J·s).

Meanwhile, the left-hand side must equate to the same units:
  • Energy-time: expressed through the units of energy (Joules) and time (seconds), leading to Joule-seconds;
  • Position-momentum: requires understanding the association of mass (kilograms), velocity (meters/second), and position (meters) to equate to Joules-seconds.

By converting physical quantities properly, verifying the unit consistency allows us to validate the equivalence of derived forms and confirms that these fundamental principles are mathematically coherent. This assures that the physical laws being studied can be correctly applied in the analysis and comprehension of natural phenomena.

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Most popular questions from this chapter

An ion having a \(4+\) charge and a mass of 49.9 u has 2 electrons with principal quantum number \(n=1,8\) electrons with \(n=2\) and 10 electrons with \(n=3 .\) Supply as many of the properties for the ion as possible from the information given. (Hint: In forming ions for this species, the 4\(s\) electrons are lost before the 3\(d\) electrons.) a. the atomic number b. total number of \(s\) electrons c. total number of \(p\) electrons d. total number of \(d\) electrons e. the number of neutrons in the nucleus f. the ground-state electron configuration of the neutral atom

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Assume that a hydrogen atom's electron has been excited to the \(n=6\) level. How many different wavelengths of light can be emitted as this excited atom loses energy?

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