/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 68 You will find in Chapter 39 that... [FREE SOLUTION] | 91Ó°ÊÓ

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You will find in Chapter 39 that electrons cannot move in definite orbits within atoms, like the planets in our solar system. To see why, let us try to "observe" such an orbiting electron by using a light microscope to measure the electron's presumed orbital position with a precision of, say, \(10 \mathrm{pm}\) (a typical atom has a radius of about \(100 \mathrm{pm}\) ). The wavelength of the light used in the microscope must then be about \(10 \mathrm{pm}\). (a) What would be the photon energy of this light? (b) How much energy would such a photon impart to an electron in a head-on collision? (c) What do these results tell you about the possibility of "viewing" an atomic electron at two or more points along its presumed orbital path? (Hint: The outer electrons of atoms are bound to the atom by energies of only a few electron-volts.)

Short Answer

Expert verified
The photon energy is too high for an orbiting electron to remain bound, making observation of its path impossible.

Step by step solution

01

Calculate the Wavelength Energy

To find the energy of a photon that has a wavelength of \(10 \mathrm{pm}\), we use the formula for photon energy: \(E = \frac{hc}{\lambda}\), where \(h\) is Planck's constant \(6.626 \times 10^{-34} \mathrm{Js}\) and \(c\) is the speed of light \(3 \times 10^8 \mathrm{m/s}\). Convert the wavelength to meters: \(\lambda = 10 \mathrm{pm} = 10^{-11} \mathrm{m}\). Substitute the values into the equation to get:\[E = \frac{(6.626 \times 10^{-34})(3 \times 10^8)}{10^{-11}} = 1.986 \times 10^{-14} \mathrm{J}\]

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Key Concepts

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

Photon Energy
Photon energy is the energy carried by a single photon, fundamentally determined by the photon's wavelength. It is crucial in understanding various phenomena in quantum mechanics and atomic interactions. To calculate the energy of a photon, we use the formula:
  • \[ E = \frac{hc}{\lambda} \]
  • Where:
    • \( E \) represents the photon energy
    • \( h \) is Planck's constant, with a value of \( 6.626 \times 10^{-34} \mathrm{Js} \)
    • \( c \) is the speed of light, approximately \( 3 \times 10^8 \mathrm{m/s} \)
    • \( \lambda \) is the wavelength of the photon
This formula highlights how energy is inversely proportional to wavelength. A shorter wavelength means higher energy, which was the case in the exercise with a wavelength of \(10 \mathrm{pm}\). This high energy can directly impact atomic structures when photons collide with electrons. It underscores that observing atomic electrons with such high-energy photons can disturb their natural state significantly. This is central to the challenges faced in visualizing or locating electrons in their orbits.
Electron Orbits
In classical models, electrons were once thought to move in fixed, predictable orbits around the atomic nucleus, somewhat similar to how planets orbit the sun. However, quantum mechanics introduces a more complex picture. Electrons do not have fixed paths but rather exist in regions of probability around the nucleus known as orbitals. Key points about electron orbits in quantum mechanics:
  • Electrons are best described by wave functions, which indicate the probability of finding an electron in a particular location around the nucleus.
  • These orbitals differ in shape and size, based on the energy level of the electron and the type of atomic orbital (e.g., s, p, d, f).
  • In quantum mechanics, the precise position and velocity of an electron cannot be simultaneously known, a principle known as the Heisenberg Uncertainty Principle.
The attempt to observe electrons in specific orbits using photons of high energy, as highlighted in the original exercise, demonstrates the disruption that these photons cause. Due to the uncertainty and the influence of observation on the system, "viewing" electrons at multiple points along a presumed orbital path is fundamentally problematic.
Planck's Constant
Planck's constant is a fundamental constant in quantum physics that characterizes the sizes of quantized units of energy. It bridges the properties of waves and particles, which is essential for understanding phenomena at the atomic and subatomic levels.Some crucial aspects of Planck's constant:
  • The value of Planck's constant is \(6.626 \times 10^{-34} \mathrm{Js}\).
  • It plays a pivotal role in the formula for photon energy, connecting the energy of photons (quantum particles of light) with their wavelength.
  • Planck's constant is integral to several fundamental quantum equations, such as the energy of a quantum of electromagnetic radiation (photon), \(E = hf\), where \(f\) is frequency.
Planck's constant helps unravel the nature of matter and light at the smallest scales, providing a foundation for the development and understanding of quantum mechanics. It serves as a constant reminder that at the quantum level, traditional physics gives way to new rules and behaviors.
Atomic Structure
Atomic structure delves into the components and arrangement of atoms, which consist of protons, neutrons, and electrons. Understanding atomic structure is crucial for grasping how matter forms and behaves. Key insights into atomic structure:
  • The nucleus of an atom contains protons, which are positively charged, and neutrons, which have no charge. The number of protons (atomic number) defines the element.
  • The electrons, which have a negative charge, are found in orbitals around the nucleus. These orbitals define the regions where electrons are most likely to be found.
  • Each element has unique electron configurations, leading to varied chemical properties and behaviors.
  • Interactions at the atomic level, such as bonding and reactions, hinge upon the arrangement and movement of these electrons.
The fundamental structure of atoms underpins much of chemistry and physics. The exercise's exploration of electron observation shows the intricate interplay of atomic components and the limits of classical models when explaining their behavior in the quantum realm.

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Most popular questions from this chapter

A stream of protons, each with a speed of \(0.9900 c\), are directed into a two- slit experiment where the slit separation is \(4.00 \times\) \(10^{-9} \mathrm{~m}\). A two-slit interference pattern is built up on the viewing screen. What is the angle between the center of the pattern and the second minimum (to either side of the center)?

An electron with total energy \(E=5.1 \mathrm{eV}\) approaches a barrier of height \(U_{b}=6.8 \mathrm{eV}\) and thickness \(L=\) \(750 \mathrm{pm}\). What percentage change in the transmission coefficient \(T\) occurs for a \(1.0 \%\) change in (a) the barrier height, (b) the barrier thickness, and (c) the kinetic energy of the incident electron?

Consider a collision between an x-ray photon of initial energy \(50.0 \mathrm{keV}\) and an electron at rest, in which the photon is scattered backward and the electron is knocked forward. (a) What is the energy of the backscattered photon? (b) What is the kinetic energy of the electron?

If the de Broglie wavelength of a proton is \(100 \mathrm{fm}\), (a) what is the speed of the proton and (b) through what electric potential would the proton have to be accelerated to acquire this speed?

(a) The smallest amount of energy needed to eject an electron from metallic sodium is \(2.28 \mathrm{eV}\). Does sodium show a photoelectric effect for red light, with \(\lambda=680 \mathrm{~nm} ?\) (That is, does the light cause electron emission?) (b) What is the cutoff wavelength for photoelectric emission from sodium? (c) To what color does that wavelength correspond?

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