Lecture Notes on Classical Mechanics for Physics 106ab – Errata
... The constraint defining rigid-body motion, |~ra − ~rb | = cab for all particles a, b in the body, is similar in form: an allowed virtual displacement keeps the length of the vector separation of the two particles fixed but allows its orientation to change, while the force that maintains the constrai ...
... The constraint defining rigid-body motion, |~ra − ~rb | = cab for all particles a, b in the body, is similar in form: an allowed virtual displacement keeps the length of the vector separation of the two particles fixed but allows its orientation to change, while the force that maintains the constrai ...
The Relativistic Quantum World
... The Story Sofar Postulates of Special Relativity Two observers in so-called inertial frames, i.e. they move with a constant relative speed to each other, observe that: 1) The laws of physics for each observer are the same, 2) The speed of light in vacuum for each observer is the same. ...
... The Story Sofar Postulates of Special Relativity Two observers in so-called inertial frames, i.e. they move with a constant relative speed to each other, observe that: 1) The laws of physics for each observer are the same, 2) The speed of light in vacuum for each observer is the same. ...
1 The Fourier Transform
... This is the time-dependent Schrödinger equation for a free particle, i.e., where V = 0, written in the position representation. This shows that plane waves exp(ikx − iωt) are eigenfunctions of the free particle Hamiltonian. The probability of finding a particle at position x is proportional to the ...
... This is the time-dependent Schrödinger equation for a free particle, i.e., where V = 0, written in the position representation. This shows that plane waves exp(ikx − iωt) are eigenfunctions of the free particle Hamiltonian. The probability of finding a particle at position x is proportional to the ...
Quantum Spin Doctors Dissect Exotic States of Matter
... both like particles and like waves. In the second, the atomic spins that are the source of the system’s mag- ridiculous at the scale of a cat in a box, it is key to the netic properties must at times be thought of as occu- Bose–Einstein condensate being studied by Dr. Roscilde and his colleagues. As ...
... both like particles and like waves. In the second, the atomic spins that are the source of the system’s mag- ridiculous at the scale of a cat in a box, it is key to the netic properties must at times be thought of as occu- Bose–Einstein condensate being studied by Dr. Roscilde and his colleagues. As ...
Quantum Chemistry and Spectroscopy
... still in a singlet state but on different atom orbital. This is marked as ...
... still in a singlet state but on different atom orbital. This is marked as ...
EOCT Challenge
... 14. Write 6.05 x 10-3m in long form. 0.00605m 15. Write 3.115 x 106km in long form. 3 115 000km 16. Calculate the volume of a room that is 3m high, 4m wide, and 6m long. V=72m3 ...
... 14. Write 6.05 x 10-3m in long form. 0.00605m 15. Write 3.115 x 106km in long form. 3 115 000km 16. Calculate the volume of a room that is 3m high, 4m wide, and 6m long. V=72m3 ...
quant-ph
... with Θ the Heaviside function and ∆E ≥ 0. A wave packet coming from the left gets partially reflected at the step and partially transmitted. The size of the reflected and the transmitted packets can be determined by a standard textbook method of calculation (e.g., [1, 2]), the stationary analysis, r ...
... with Θ the Heaviside function and ∆E ≥ 0. A wave packet coming from the left gets partially reflected at the step and partially transmitted. The size of the reflected and the transmitted packets can be determined by a standard textbook method of calculation (e.g., [1, 2]), the stationary analysis, r ...
Chapter 3
... When a solid is heated, it emits electromagnetic radiation, known as blackbody radiation, over a wide range of wavelengths. The amount of energy given off at a certain temperature depends on the wavelength. Classical physics failed to completely explain the phenomenon. Assumed that radiant energy ...
... When a solid is heated, it emits electromagnetic radiation, known as blackbody radiation, over a wide range of wavelengths. The amount of energy given off at a certain temperature depends on the wavelength. Classical physics failed to completely explain the phenomenon. Assumed that radiant energy ...
Chapter 5 * Electrons in Atoms
... • Atoms can emit light when you add heat, electricity, or reaction energy. • The electrons start at ground state. When they absorb energy, they jump to a higher energy level (excited state). • They have to lose the energy to fall back to ground state, and they lose some of that energy in the form o ...
... • Atoms can emit light when you add heat, electricity, or reaction energy. • The electrons start at ground state. When they absorb energy, they jump to a higher energy level (excited state). • They have to lose the energy to fall back to ground state, and they lose some of that energy in the form o ...
01-4-momentum-with
... depends on the mass of the cart. Both mass and the velocity of the cart are important. ...
... depends on the mass of the cart. Both mass and the velocity of the cart are important. ...
L5 QM wave equation
... But before we continue, we note that Schrödinger’s idea of a “matter wave” for electrons turned out to be totally unworkable. Just think about the electric charge of an electron: if an electron is really a matter wave, then we should be able to find bits of its charge in different places. No such bi ...
... But before we continue, we note that Schrödinger’s idea of a “matter wave” for electrons turned out to be totally unworkable. Just think about the electric charge of an electron: if an electron is really a matter wave, then we should be able to find bits of its charge in different places. No such bi ...
Physics 3 for Electrical Engineering
... But before we continue, we note that Schrödinger’s idea of a “matter wave” for electrons turned out to be totally unworkable. Just think about the electric charge of an electron: if an electron is really a matter wave, then we should be able to find bits of its charge in different places. No such bi ...
... But before we continue, we note that Schrödinger’s idea of a “matter wave” for electrons turned out to be totally unworkable. Just think about the electric charge of an electron: if an electron is really a matter wave, then we should be able to find bits of its charge in different places. No such bi ...
