• Study Resource
  • Explore
    • Arts & Humanities
    • Business
    • Engineering & Technology
    • Foreign Language
    • History
    • Math
    • Science
    • Social Science

    Top subcategories

    • Advanced Math
    • Algebra
    • Basic Math
    • Calculus
    • Geometry
    • Linear Algebra
    • Pre-Algebra
    • Pre-Calculus
    • Statistics And Probability
    • Trigonometry
    • other →

    Top subcategories

    • Astronomy
    • Astrophysics
    • Biology
    • Chemistry
    • Earth Science
    • Environmental Science
    • Health Science
    • Physics
    • other →

    Top subcategories

    • Anthropology
    • Law
    • Political Science
    • Psychology
    • Sociology
    • other →

    Top subcategories

    • Accounting
    • Economics
    • Finance
    • Management
    • other →

    Top subcategories

    • Aerospace Engineering
    • Bioengineering
    • Chemical Engineering
    • Civil Engineering
    • Computer Science
    • Electrical Engineering
    • Industrial Engineering
    • Mechanical Engineering
    • Web Design
    • other →

    Top subcategories

    • Architecture
    • Communications
    • English
    • Gender Studies
    • Music
    • Performing Arts
    • Philosophy
    • Religious Studies
    • Writing
    • other →

    Top subcategories

    • Ancient History
    • European History
    • US History
    • World History
    • other →

    Top subcategories

    • Croatian
    • Czech
    • Finnish
    • Greek
    • Hindi
    • Japanese
    • Korean
    • Persian
    • Swedish
    • Turkish
    • other →
 
Profile Documents Logout
Upload
Lecture 5 - Ultra high energy cosmic rays and the GZK cutoff
Lecture 5 - Ultra high energy cosmic rays and the GZK cutoff

10.5.1. Density Operator
10.5.1. Density Operator

... When dealing with a large quantum system, we need to take 2 averages, one over the inherent quantum uncertainties and one over the uninteresting microscopic details. Consider then an isolated system described, in the Schrodinger picture, by a complete set of orthonormal eigenstates  n  t  ...
CHAPTER 5
CHAPTER 5

... electrons in the same atom can have the same set of quantum #’s • 3. Hund’s Rule- orbitals of equal energy are each occupied by 1 electron before any orbital is occupied by a second electron • all electrons in single occupied orbitals must have the same spin ...
1) Which of the following concepts was discussed in Chapter 1
1) Which of the following concepts was discussed in Chapter 1

... Q17) A particle in a certain finite potential energy well can have any of five quantized energy values and no more. Which of the following would allow it to have any of six quantized energy levels? 1) Increase the momentum of the particle 2) Decrease the momentum of the particle 3) Decrease the well ...
CHEM3023: Spins, Atoms and Molecules
CHEM3023: Spins, Atoms and Molecules

i∂φ
i∂φ

TED
TED

QUANTUM NUMBERS
QUANTUM NUMBERS

Quantum Mechanics from Periodic Dynamics: the bosonic case
Quantum Mechanics from Periodic Dynamics: the bosonic case



Sections 5 - Columbia Physics
Sections 5 - Columbia Physics

CHAPTER 7: The Hydrogen Atom
CHAPTER 7: The Hydrogen Atom

... the z-component Lz are constant while the x and y components can take a range of values and average to zero, just like the quantum eigenfunctions. A given quantum number l determines the magnitude of the vector L via ...
Document
Document

Diode Pumped Solid State
Diode Pumped Solid State

... In equilibrium, the charge carriers occupy their lowest energy states, electrons at the bottom of the conduction band, and holes at the top of the valence band. In silicon these states do not have the same momentum. Therefore if a recombination is to result in the emission of a photon, which has lit ...
Section 1 Notes
Section 1 Notes

Chapter 10 • We want to complete our discussion of quantum Schr
Chapter 10 • We want to complete our discussion of quantum Schr

... algebra to solve for Ψ(x) the way we would solve for a variable “y”.  This equation describes how the function must behave at all x!  There are techniques for solving differential equations but they are not generalized…they depend on the form of the differential equation.  The best we can do here ...
Chemistry - Unit 6 What do you need to know?? This chapter is on
Chemistry - Unit 6 What do you need to know?? This chapter is on

... It was Einstein, in 1905, who deduced the basis of the photoelectric effect. I like an example that Dr. Blaber, at Florida State University uses: The Photoelectric effect as a carnival game: "A popular carnival game is where you are given a giant mallet and have to hit a pad on the ground. This send ...
A Simply Regularized Derivation of the Casimir Force
A Simply Regularized Derivation of the Casimir Force

QUIZ
QUIZ

... c. The Magnetic Quantum Number is the electrons three dimensional position in space d. The Spin Quantum Number is the direction of the electrons spin 43. I listed the first four orbital shapes for the orbital quantum number. What are the four letters that represent these four shapes. (4 points) s, p ...
Advanced Quantum Physics - Theory of Condensed Matter
Advanced Quantum Physics - Theory of Condensed Matter

ps700-coll2-hayden
ps700-coll2-hayden

... Niels Bohr was working on quantum mechanics in an era where it was already a well established theory (1924-26). Professor Al-Khalili actually compared Bohrs’ genius to that of Einstein’s but said that “Bohr was however a very bad talker, not a very good lecturer and although a good footballer, not ...
Chapter 6 Concept Tests
Chapter 6 Concept Tests

41 Chapter 4 Atomic Structure 4.1 The Nuclear Atom J. J. Thomson
41 Chapter 4 Atomic Structure 4.1 The Nuclear Atom J. J. Thomson

Quantum Mechanics Problem Set
Quantum Mechanics Problem Set

... (a) The uncertainty principle states that there is a limit to how precisely we can simultaneously know the position and momentum (a quantity relates to energy) of an electron. The Bohr model states that electrons move about the nucleus in precisely circular orbits of known radius and energy. This vi ...
Physics 610: Quantum Optics
Physics 610: Quantum Optics

... from the University of Rochester published a treatise that encompasses a very broad range of topics, both in the classical and quantum theories of light. Topics on the classical theory of light propagation and on the coherence of light, the research specialty of Wolf, are treated in detail in the fi ...
< 1 ... 242 243 244 245 246 247 248 249 250 ... 329 >

Particle in a box



In quantum mechanics, the particle in a box model (also known as the infinite potential well or the infinite square well) describes a particle free to move in a small space surrounded by impenetrable barriers. The model is mainly used as a hypothetical example to illustrate the differences between classical and quantum systems. In classical systems, for example a ball trapped inside a large box, the particle can move at any speed within the box and it is no more likely to be found at one position than another. However, when the well becomes very narrow (on the scale of a few nanometers), quantum effects become important. The particle may only occupy certain positive energy levels. Likewise, it can never have zero energy, meaning that the particle can never ""sit still"". Additionally, it is more likely to be found at certain positions than at others, depending on its energy level. The particle may never be detected at certain positions, known as spatial nodes.The particle in a box model provides one of the very few problems in quantum mechanics which can be solved analytically, without approximations. This means that the observable properties of the particle (such as its energy and position) are related to the mass of the particle and the width of the well by simple mathematical expressions. Due to its simplicity, the model allows insight into quantum effects without the need for complicated mathematics. It is one of the first quantum mechanics problems taught in undergraduate physics courses, and it is commonly used as an approximation for more complicated quantum systems.
  • studyres.com © 2025
  • DMCA
  • Privacy
  • Terms
  • Report