Physics
- 1800. William Herschel discovers infrared radiation.
- 1801. Double-slit experiment demonstrates wave-particle duality. By Thomas Young.
- 1814. Fraunhofer lines are the spectral absorption lines of the sun.
- 1853. Anders Angstrom shows that the spectrum of an electric spark superposes the spectra of the electrode metal and the gas.
- 1859. John Tyndall measures infrared absorption by gases.
- 1860. Black-body radiation and the laws of spectroscopy by Gustav Kirchhoff and Bunsen. Stellar spectral lines are due to absorption.
- 1860. Robert Bunsen and Gustav Kirchhoff discover caesium and rubidium.
- 1894. Lord Rayleigh discovers argon. 1904 Nobel Prize.
- 1896. Wilhelm Röntgen discovers X-rays. 1901 Nobel Prize, the first.
- 1896. Henri Becquerel discovers radioactive decay in uranium and thorium. He thought phosphorescent materials might emit X-rays that could penetrate black paper, but found that the result was due to radioactivity. Marie Curie uses an electrometer to measure the conductivity of air and shows that radioactivity depends only on the quantity of uranium.
- 1896. Zeeman effect: spectral lines split into several components in a magnetic field. By Pieter Zeeman and Hendrik Lorentz. 1902 Nobel Prize.
- 1898. Marie Curie and Pierre Curie discover polonium and radium. Becquerel and the Curies receive the 1903 Nobel Prize. Marie wins the 1911 Nobel Prize in Chemistry after Pierre died. Marie dies of anemia.
- 1900. Max Planck discovers quantization and Planck’s constant. 1918 Nobel Prize.
- 1903. Rutherford models the half-life of radioactive decay and wins the 1908 Nobel Prize in Chemistry.
- 1903. Frederick Soddy shows that the decay of radium produces helium. 1921 Nobel Prize in Chemistry.
- 1910. Millikan oil-drop experiment measures electric charge. 1923 Nobel Prize.
- 1911. Rutherford scattering experiments discover the nucleus by measuring the deflection of alpha particles passing through a thin gold foil. Rutherford model of the atom with a small charged nucleus containing most of its mass.
- 1912. Victor Hess discovers cosmic rays. Measures ionization with Wulf electrometers in a balloon during a solar eclipse to rule out the sun as a source. 1936 Nobel Prize.
- 1913. Bohr model of the atom where electrons have discrete energy levels. 1922 Nobel Prize.
- 1914. Percy Bridgman studies the physics of high pressure, up to 10 GPa. Bridgman seal. 1946 Nobel Prize.
- Black phosphorus is a 2D pleated honeycomb structure and the most stable form.
- 1922. Stern-Gerlach experiment shows that spin is quantized.
- 1923. Compton scattering demonstrates the particle nature of electromagnetic radiation. 1927 Nobel Prize.
- 1924. Pauli exclusion principle. 1945 Nobel Prize.
- 1924. Louis de Broglie predicts matter waves. 1929 Nobel Prize.
- 1925. Werner Heisenberg creates quantum mechanics, including the Heisenberg uncertainty principle in 1927. 1932 Nobel Prize. Also develops the S-matrix in 1944.
- 1926. Schrödinger equation. 1933 Nobel Prize.
- 1928. Geiger counter.
- 1927. Born-Oppenheimer approximation for wavefunctions. Assumes separable motion of nuclei and electrons, computing electronic energies for a grid of fixed nucleus positions. Molecular energy decomposes into electronic, vibrational, rotational, and nuclear spin, which is very spall. Electronic energy includes kinetic, interelectronic repulsion, internuclear repulsion, and electron-nuclear attractions.
- 1929. Dirac equation describes fermions.
- Gross structure models energy levels or spectral lines using quantum mechanics and the principal quantum number n.
- Fine structure is the splitting of spectral lines due to relativistic and spin effects.
- The Principles of Quantum Mechanics (1930).
- 1931. Wigner’s theorem says that all physical symmetries on H are unitary or antiunitary transformations. Wigner D-matrix in 1927. Half of the 1963 Nobel Prize.
- 1931. Ernest Lawrence invents the cyclotron. 1939 Nobel Prize.
- 1932. James Chadwick discovers the neutron. 1935 Nobel Prize.
- 1932. Carl David Anderson discovers the positron. 1936 Nobel Prize. Also discovers the muon in 1936.
- 1934. Harold Urey discovers deuterium. 1934 Nobel Prize in Chemistry.
- 1934. Induced radioactivity discovered by Irène Joliot-Curie and Frédéric Joliot-Curie using alpha particles. 1935 Nobel Prize in Chemistry.
- 1934. Enrico Fermi shows neutron-induced radioactivity and claims to have created transuranic elements. 1938 Nobel Prize. Ida Noddack correctly hypothesizes nuclear fission.
- 1934. Cherenkov radiation by Pavel Cherenkov, Ilya Frank, and Igor Tamm. 1934 Nobel Prize.
- 1934. Fusion between deuterium atoms at 100 keV.
- 1935. Hideki Yukawa publishes a field theory and predicts the pi meson or pion. 1949 Nobel Prize.
- 1938. Nuclear fission splits the atom. German chemists Otto Hahn and Fritz Strassmann bombard uranium with slow neutrons. 1944 Nobel Prize in Chemistry. Physicist Lise Meitner and her nephew Otto Frisch develop the theory.
- 1939. Stellar nucleosynthesis and the CNO cycle by Hans Bethe. 1967 Nobel Prize.
- 1939. Black holes predicted by the Oppenheimer-Snyder model. Tolman-Oppenheimer-Volkoff limit on the mass of cold, non-rotating neutron stars.
- 1940. Neptunium is the first transuranium element. Edwin McMillan and Glenn Seaborg use reduction and oxidation. 1951 Nobel Prize. Seaborg develops the actinide series.
- 1943. Girdler sulfide process extracts deuterium from water. By Karl-Hermann Geib and Jerome S. Spevack. In H2O + HDS ⇌ HDO + H2S, the cold tower produces 15% D2O. Further enrichment requires distillation.
- 1947. Lamb shift: quantum states of hydrogen atoms had slightly more energy than predicted by the Dirac equation. 1955 Nobel Prize with Polykarp Kusch, who determines the magnetic moment of the electron is greater than its theoretical value.
- 1947. Pion by C. F. Powell. 1950 Nobel Prize.
- 1948. Quantum electrodynamics and renormalization: 1965 Nobel Prize.
- Julian Schwinger: the Schwinger model, the first theory of confinement in 1+1 dimensions; Schwinger’s quantum action principle, a variational approach; and an electroweak gauge theory.
- Shinichiro Tomonaga
- Feynman diagram to represent particle interactions.
- propagator is the probability amplitude for a particle to travel with a certain momentum or location.
- Annihilation is a collision between a particle and its antiparticle.
- 1949. Freeman Dyson systematizes renormalization.
- 1949. Ramsey interferometry uses magnetic resonance and oscillating electromagnetic fields to measure transition frequencies. Half of the 1989 Nobel Prize.
- 1952. Bubble chamber by Donald A. Glaser. 1960 Nobel Prize.
- 1953. Maser and laser by Charles Townes, Nikolay Basov and Alexander Prokhorov. 1964 Nobel Prize. Laser built by Theodore Maiman in 1960.
- Laser gain medium like GaAs or GaN amplifies power. Crystals, glasses, and ceramics can also be doped with trivalent rare earth ions like Nd, Yb, or Er. Thermal lensing: higher temperature on the beam axis causes a radial gradient in the refractive index (thermooptic effect), causing focusing.
- 1955. Antiproton by Emilio Segre and Owen Chamberlain. 1959 Nobel Prize.
- 1955. Luis Walter Alvarez scales up the bubble chamber and discovers particle resonance states. 1968 Nobel Prize.
- 1955. Quadrupole ion trap and Penning trap Wolfgang Paul and Hans Georg Dehmelt, used to measure the electron magnetic moment. Half of the 1989 Nobel Prize. Also quadrupole mass analyzer.
- 1956. Clyde Cowan and Frederick Reines discover the neutrino.
- 1956. Chen-Ning Yang and Tsung-Dao Lee show that parity symmetry was not conserved in the weak interaction. 1957 Nobel Prize. Confirmed by Chien-Shiung Wu.
- 1968. Raymond Davis and Masatoshi Koshiba detect solar neutrinos and the solar neutrino problem. Half of the 2002 Nobel Prize.
- 1970. radio-frequency quadrupole (RFQ) linear accelerator.
- 1987. Electron beam ion trap (EBIT).
- 1998. Neutrino oscillation confirmed by Takaaki Kajita and Arthur McDonald. 2015 Nobel Prize. Oscillation changes in matter, the Mikheyev-Smirnov-Wolfenstein (MSW) effect.
- 1999. Chandra X-ray Observatory by Riccardo Giacconi. Half of the 2002 Nobel Prize.
Manhattan Project
- Elizabeth Riddle Graves worked on fast neutron scattering, nuclear cross-sections, neutron reflectors, and chain reaction calculations.
- 1939. Einstein-Szilard letter to FDR recommends a nuclear weapon program.
- 1942. Chicago Pile-1 by Enrico Fermi is the first artificial nuclear chain reaction.
- Leona Woods builds boron trifluoride detectors to measure neutron flux.
- 1942. Leslie Groves drives the project.
- 1943. Robert Oppenheimer is director of Los Alamos. Spiritual and interested in Hindu religion. Hans Bethe leads the T Division on theory and works on implosion hydrodynamics. Enrico Fermi leads the F Division.
- 1943. Quebec Agreement pools resources with the British Tube Alloys project.
- Hanford Site is the first plutonium production reactor.
- Y-12 in Oak Ridge, Tennessee enriches uranium.
- electromagnetic coils used 14,700 tons or $300 million of silver. Less than 0.036% was lost.
- “Colonel, in the Treasury we do not speak of tons of silver; our unit is the troy ounce.”
- Calutron Girls work for the Eastman Chemical Company monitoring calutrons, sector mass spectrometers that separate uranium ions.
- S-50 enriches uranium to 2% by liquid thermal diffusion or thermophoresis: heavy molecules move to colder regions.
- 1945. Uranium is enriched by Gaseous diffusion at K-25. Forces UF6 gas through micropore membranes, with enrichment factor 1.0043.
- Graham’s law: the rate of effusion (escape) is proportional to the square root of its molecular mass.
- Fission bomb
- 1945. Trinity nuclear test: 64 kg of 80% enriched uranium-235 in two subcritical pieces. Implosion-type pit has 6.2 kg of plutonium-239 surrounded by a U-238 tamper reflects neutrons. 25 kilotons of TNT at 20% yield. Aluminum pusher lengthens the shockwave.
- John von Neumann calculates explosive lenses.
- Little Boy: gun-type fission weapon. 15 kilotons of TNT.
- Fat Man: 3 tons of high explosives for implosion.
- 1945. Alsos Mission seizes German nuclear program material, with Operation Big in southwestern Germany. Operation Epsilon detains and secretly records top German physicists at Farm Hall.
- 1946. Atomic Energy Act establishes the US Atomic Energy Commission to manage nuclear weapons. Also ends nuclear cooperation with Britain.
- 1949. boosted fission weapon uses fusion reactions to release neutrons that improve fissile yield. Reduces the confinement time needed, allowing much less conventional explosive and smaller warheads.
- Thermonuclear weapon or hydrogen bomb uses a nuclear fission primary stage and a secondary fusion stage containing deuterium or lithium deuteride.
- Teller-Ulam design. One of the Martians, Jewish-Hungarian scientists.
- 1954. Castle Bravo is the most powerful at 15 Mt TNT. Bikini Atoll, Marshall Islands. Uranium tamper undergoes dirty fission reactions leading to high fallout.
- 1952. British Operation Hurricane test in the High Explosive Research project.
- 1953. Soviet Zippe-type gas centrifuge enriches uranium-235. Developed by German scientists working in detention. 20 cm diameter spinning at 1,500 rps by electric motor. Sits on a conical jewel bearing during startup, and has a magnetic bearing on top. Feed, product, and tails gas lines. Molecular pump maintains a vacuum around the rotor.
- 1954. Oppenheimer security clearance hearing revokes his Q clearance due to his associations with communists and his peace advocacy. Atomic Energy Commission chair Lewis Strauss organizes the hearing. Strauss later loses Senate confirmation for secretary of commerce in 1959. Teller is the only scientist to testify against Oppenheimer.
- 1943. George Eltenton hosts a Soviet diplomat Piotr Ivanov, who solicits nuclear secrets. Eltenton asks Chevalier to ask Oppenheimer, who declines but fails to report it.
- 1958. US-UK Mutual Defence Agreement resumes nuclear cooperation with Britain.
Classical mechanics
International System of Units (SI) has seven base units: second, meter, kilogram, ampere, kelvin, mole, and candela. Based on the metre-kilogram-second (MKS) system.
Buckingham π theorem: an equation of n variables in k dimensions can be rewritten in terms of n-k dimensionless parameters. For example f(s, kg, m, m/s^2) is 4 variables in 3 dimensions, so we have the dimensionless quantity gT^2/L = 4π^2. Thus a pendulum has period T = 2π sqrt(L/g).
Kinematics studies the geometry of motion, excluding forces and masses.
- Rotation.
- Rotation matrix R satisfies R^T R = RR^T = I.
- In two dimensions, R = cos -sin sin cos reprsents a rotation by a counterclockwise angle.
- Tait–Bryan angles define rotations around fixed axes: Z (yaw) * Y (pitch) * X (roll). For aircraft, yaw is often defined as a counterclockwise rotation or clockwise rotation with a negative y axis.
- Gimbal lock occurs in a telescope or theodolite or three ring gyro. A gimbal cannot follow a continuous motion with continuous motion in gimbal angles: e.g. helicopter flies to the zenith immediately above the telescope, changes direction, and flies away at a different angle. At the zenith, spherical angles do not define a coordinate chart, a homeomorphism of the neighborhood with R^n.
- Euler angles use the same axis for the first and third rotation, so the line of nodes is an intersection between homologous. Apply a precession, nutation, and intrinsic rotation. This is a mixed axes of rotation system where the latter rotation operators depend on the precession.
- Euler’s rotation theorem says any rotation R has an Euler axis e (a unit vector) with eigenvalue 1: Re = R. An infinitesimal rotation dθ about e (x, y, z) has matrix ΔR = I + Adθ for A = \([0 z -y] [-z 0 x] [y -x 0]\). Integrating, we see that R = exp(Aθ), so Aθ is the generator of the rotation. The exponential map from the Lie algebra so(3) to the Lie group SO(3).
- Kinematic constraints
- Holonomic constraints
- Pendulum: |x|^2 = L^2
- Rigid body: |x_1 - x_2|^2 = L^2
Newtonian mechanics studies force as a vector. Newton’s laws of motion:
- Inertia: objects have constant velocity without external forces. There is no privieged inertial frame.
- F = ma.
- Conservation of momentum.
- Torque
- Moments
- Work W = F∙d
- Energy
- Pressure is force per area.
Newton’s law of universal gravitation: F = G m_1m_2/r^2, where the gravitational constant G = 7e-11 N m2/kg2.
Forces: normal force, friction, gravity. Projectile motion, inclined planes, circular motion and centripetal acceleration.
- Coriolis force or Coriolis effect: objects in motion in a rotating reference frame experience a fictious centrifugal force.
Harmonic motion
- Hooke’s law. The elastic force F = -kx for stiffness k and spring displacement x.
- For mass m, x(t) = A cos(wt) where frequency w = sqrt(k/m).
- A directionally stable vehicle produces a restoring moment against a rotational disturbance.
Lagrangian mechanics
- Lagrangian L = T - V for kinetic energy T and potential energy V.
- The stationary-action principle states that trajectories are stationary points of the system’s action functional, the integral of the Lagrangian between two instants in time.
- Generalized coordinates describe the configuration in configuration space.
- Particle has the configuration space R^3.
- Rigid body has the configuration space R^3 x SO(3).
- Lagrange equation.
https://archive.org/details/physicsforentert035428mbp
Thermodynamics
Some math at Thermo.
- 1625. Italian physiologist Santorio Santorio invents the thermometer, based on thermal expansion of air.
- 1629. Galileo’s student Joseph Solomon Delmedigo invents the alcohol thermometer.
- 1662. Boyle’s law that PV is constant.
- 1714. Daniel Gabriel Fahrenheit invents the mercury thermometer and a standard temperature scale.
- 1742. Anders Celsius proposes a scale based on the boiling and freezing point of water.
- 1777. Swiss pharmaceutical chemist Carl Wilhelm Scheele distinguishes thermal radiation from convection and conduction.
- 1822. Joseph Fourier discovers Fourier series, Fourier analysis and harmonic analysis, and the greenhouse effect.
- 1824. Sadi Carnot models the heat engine and the Carnot cycle.
- 1834. Émile Clapeyron expands Carnot’s work and plots it on a PV diagram.
- 1843. James Prescott Joule determines the mechanical equivalent of heat.
- 1848. Lord Kelvin proposes an absolute temperature scale and determines absolute zero.
- 1850. Rudolf Clausius states the second law of thermodynamics and entropy.
- 1859. William Rankine proposes the Rankine scale. Also the Rankine-Hugoniot conditions for shock waves normal to oncoming 1D flow.
- 1866. Maxwell-Boltzmann distribution.
- 1926. Einstein refrigerator with no moving parts.
Ideal gas law. PV = nRT.
In information theory, entropy H = -int p log p.
In statistical mechanics, entropy S = k_B * ln(W), where W is the number of microstates consistent with the observed thermodynamic state.
Gibbs entropy S = k_B * H, where H is the entropy of the Maxwell–Boltzmann distribution, in nats.
- Mean kinetic energy per particle E = 3/2 k_B T.
Change in entropy dS = dQ/T, so Q = integral dQ = integral T dS
- Temperature T = dQ/dS = dE/dS assuming no mechanical work.
- 1951. Negative temperature occurs in systems with bounded phase space where adding heat decreases entropy. It is very hot and will transfer energy to any system at positive temperature upon contact.
A reversible process does not generate entropy (frictionless, etc).
An ideal cycle is reversible, so net work equals the net heat transfer Q = Q_H - Q_C. The Carnot efficiency eta = work / Q_H = 1 - T_C / T_H.
First law of thermodynamics. Conservation of energy (heat and work). Implies that perpetual motion is impossible.
Second law of thermodynamics. Entropy always increases, or equivalently heat cannot flow spontaneously from cold to hot. Implies Carnot’s theorem that the maximum efficiency of a heat engine is the Carnot efficiency.
- Loschmidt’s paradox. Time-symmetric dynamics cannot explain an irreversible process.
Third law of thermodynamics. Entropy S = 0 for a perfect crystal at absolute zero. The ground state is a unique state with minimum energy.
1929. Onsager reciprocal relations relate flows in non-equilibrium systems and irreversible processes. 1968 Nobel Prize in Chemistry.
- heat flow per pressure difference and the density flow per temperature difference are equal due to microscopic time reversibility.
Temperature |
Thermal conduction |
Seebeck effect |
Soret effect (thermophoresis) |
Voltage |
Peltier effect |
Ohm’s law |
Electromigration |
Chemical potential |
Dufour effect |
Galvanic cell |
Fick’s law |
Stress |
Thermoelasticity |
Piezoelectricity |
Osmosis |
An adiabatic process occurs without heat exchange between the system and its environment.
Carnot cycle: Q = delta T * delta S.
- Isothermal expansion: W out, Q in, decreases P, increases V.
- Adiabatic expansion: W out, decreases T, decreases P, increases V.
- Isothermal compression: W in, Q out, increases P, decreases V.
- Adiabatic compression: W in, increases T, increases P, decreases V.
Stirling cycle:
- Isothermal expansion: W out, Q in, decreases P, increases V
- Isovolumetric cooling: Q out, decreases P
- Isothermal compression: W in, Q out, increases P, decreases V
- Isovolumetric heating: Q in, increases P
Rankine cycle for steam engines: uses lower temperature steam input
- Isobaric heating: Q in
- Adiabatic expansion: W out, decreases P, increases V
- Isobaric cooling: Q out
- Adiabatic compression: W in, increases P, decreases V
Brayton cycle for gas turbines and jet engines:
- Isobaric expansion: Q in, increases V
- Adiabatic expansion: W out, decreases P, increases V
- Isobaric compression: Q out
- Adiabatic compression: increases P, decreases V
Diesel cycle: high efficiency, low stress.
- Isobaric heating: Q in, increases V
- Adiabatic expansion: W out, decreases P, increases V
- Isovolumetric cooling: Q out
- Adiabatic compression: W in, increases P, decreases V, ignites the fuel.
Otto cycle: gasoline engine.
- Isovolumetric heating: Q in (burn fuel), increases P
- Adiabatic expansion: power stroke
- Isovolumetric cooling: Q out, decreases P
- Adiabatic compression
Refrigeration
Irreversible cycles:
Vapor-compression refrigeration consists of a compressor, condenser, expansion valve, and an evaporator.
- Adiabatic compression: W in, increases T and P
- Hot vapor condenses to a hot liquid: Q out.
- Hot liquid is isenthalpically expanded using a thermal expansion valve (aka throttle valve) to become cold (and partly gas).
- Cold liquid evaporates to become gas, Q in.
Joule–Thomson effect that most gases cool (positive JT coefficient) and most liquids warm up when expanding: used in the Siemens cycle and Hampson–Linde cycle. Irreversible.
https://en.wikipedia.org/wiki/De_Laval_nozzle
Siemens cycle uses the
- Compress the gas to increase temperature.
- Cool gas by exchanging with environment.
- Cool gas by expanding the gas and doing work.
Hampson–Linde cycle is used to liquefy gases with regenerative cooling.
https://en.wikipedia.org/wiki/Hampson%E2%80%93Linde_cycle
https://en.wikipedia.org/wiki/Regenerative_cooling
https://en.wikipedia.org/wiki/Dilution_refrigerator
Absorption refrigerator such as the Einstein refrigerator.
- A mixed fluid is heated so the ammonia refrigerant evaporates out. (Hydrogen is used for pressure balance.)
- Refrigerant condenses, releasing heat to the environment.
- Refrigerant evaporates (absorbing heat) by being absorbed into water.
Dilution refrigerator cools to 2 mK
Sisyphus cooling
Heat equation and diffusion equation are parabolic.
Fluid and continuum mechanics
See also acoustic engineering.
Density and pressure. Buoyant Force and Archimedes’ Principle.
Bernoulli’s principle is the conservation of energy for flows. For incompressible flows, the sum of static pressure, dynamic pressure (kinetic energy), and hydraulic head (gravitational energy) is invariant.
- The head at the top of a weir provides a direct measurement of the flow rate.
Pitot tube measures stagnation pressure (or total pressure where gravity is not a factor). It is a tube pointing into the flow of liquid and closed at the other end, to convert all the fluid velocity to static pressure.
Venturi effect. In a constricted pipe, velocity increases proportional to the decrease in cross-sectional area, and the increase in kinetic energy causes a decrease in static pressure. A differential pressure sensor can measure fluid velocity.
- In a choked flow, the fluid velocity reaches the speed of sound, and any further decrease in the downstream pressure environment does not affect velocity. For a compressible gas, increasing upstream pressure will increase density and mass flow rate.
- A carburetor uses the Venturi effect to suction fuel by blowing air through a constriction
Viscosity μ is the internal friction force between layers in relative motion.
- Shear viscosity or dynamic viscosity (in Pa·s or kg/m/s).
- Shear stress τ = F/A = μ du/dy for a velocity gradient du/dy.
- Kinematic viscosity ν = μ/ρ (in m^2/s).
- Volume viscosity measures irreversible resistance to compression. Compare bulk modulus, which is reversible.
- Reynolds number is a ratio between inertial and viscous forces.
- Laminar flow has low Reynolds number, while turbulent flow has high Reynolds number.
- R = uL/ν for speed u, characteristic length L, and kinematic viscosity ν.
- Characteristic length or hydraulic diameter is cross section area / wetted perimeter.
- Stoke’s law: Stoke’s drag F = 6πμRv for a sphere of radius R in a laminar flow with velocity v.
- Couett flow models a viscous fluid between a stationary and a moving surface.
- A Newtonian fluid has a constant viscosity, implying that viscous stress is linearly proportional to the local strain rate.
- Incompressible flow: shear stress τ = μ (∇u + ∇u.T) for velocity gradient ∇u.
- Non-Newtonian fluids include:
- shear-thinning: most biological fluids, ketchup, quicksand
- shear-thickening oobleck (cornstarch)
- Weissenberg effect: liquid is drawn towards a spinning rod (hoop stress)
- Maxwell material: elastic resistance to fast deformations, such as slime
- Coandă effect: a fluid jet tends to attach to a nearby surface. A fluid jet entrains fluid from the surroundings, developing a region of lower pressure. When one side is a surface, ambient pressure creates a net force on the fluid jet towards the surface.
- https://en.wikipedia.org/wiki/Hydraulic_jump
Navier-Stokes equations describe the motion of viscous fluids.
- A solution is a flow velocity vector field.
- Streamlines are field lines in fluid flow and show the path a massless particle would take.
- No-slip-condition states that viscous fluid has zero velocity at a solid boundary.
Fluid dynamics
- Continuity equation: flow q = Av for area A and velocity v
- wave equation: $ = c^2 .
- Shallow water equations
- Euler equations
- Manning formula estimates average velocity in an open channel flow.
- V = 1/n R^(2/3) S^(1/2) for hydraulic radius R, slope S, and coefficient n = 1 s/m^(1/3)
- Standard step method estimates 1D water depth profile in a steady state open channel
- E-y diagram: energy (total head) vs. flow depth
- critical depth is the depth with minimum energy.
- Froude number Fr = u/sqrt(gL). Dimensionless ratio of flow inertia to gravity, with flow velocity u (m/s).
- HEC-RAS: Hydrologic Engineering Center River Analysis System
- HBV hydrology model
- Snow: melting temperature threshold (TT), melt rate Cmelt
- Soil moisture field capacity FC
- initial precipitation -> infiltration + evapotranspiration + runoff into surface reservoir S1 -> percolation rate Kd plus fast flow K2 above threshold L -> groundwater S2 -> K2 -> flow Q3.
- Evapotranspiration (ETP) from permanent wilting point (PWP) and C (ETP increase per temperature).
- Storm Water Management Model (SWMM)
Doppler effect: change in frequency due to relative motion. Light sources moving away at relativistic speeds are redshifted.
Slosh dynamics model liquid momentum, inertial waves, and resonance. A slack tank has a free surface is subject to zero parallel shear stress. The free surface effect can cause boats to capsize. Mitigate using baffles.
Pumps
- centrifugal pump: more powerful for high-density fluids
- axial-flow pump: better for low-density fluids like liquid hydrogen. Much higher volumetric flowrate, smaller diameter, lower pressure increase.
- The Scallop theorem says that a reciprocal motion cannot achieve net displacement in a low-Reynolds number Newtonian fluid.
- Power number: P/(ρ n^3 D^5) for power P, density ρ (kg/m^3), rotor diameter D, angular speed n (Hz).
https://en.wikipedia.org/wiki/Turbine
Impulse turbine: change the direction of flow, reduces kinetic energy. Pressure drop at nozzle, and no pressure change in the turbine blades. Useful for low flow and high head.
Reaction turbine: pressure changes as it passes the turbine rotor blades. Useful for high velocity and low head.
For a turbine, the degree of reaction is the ratio of the static pressure drop in the blades to total pressure drop in the stage. An impulse turbine only has a stator.
A Pelton wheel is an impulse water turbine where water flows into and turns spoon-shaped buckets. It is optimal for high hydraulic head and low flow rates.
Ships
A ducted propeller improves thrust at very low speeds (tugs and trawlers).
TODO Kort nozzle
Surface ships use waterjets with outlet above the waterline and axial flow impellers. Cavitation occurs at
A pumpjet is integrated behind the hull, axial duct, and stator to reduce rotational energy output. Lower internal pressure (due to higher internal velocity) allows higher speed before cavitation.
An azimuth thruster or azipod can rotate horizontally. It is more maneuverable than a rudder.
harbor pilot
mooring lines to the dock
whitecaps 20 knots
https://en.wikipedia.org/wiki/Fluid_mechanics
https://en.wikipedia.org/wiki/Template:Rivers,_streams_and_springs
https://en.wikipedia.org/wiki/Template:Agricultural_water_management
https://en.wikipedia.org/wiki/Template:Agricultural_water_management_models
Optics
Spectrum: radio, microwave, infrared, visible, ultraviolet, X-ray, gamma ray. Earth atmosphere is visible to radio and visible radiation.
- Ultraviolet
- UV‑A 315-400 nm, blacklight is usually a fluorescent bulb.
- Violet filter allows a dim violet glow
- Can cause melanoma via indirect DNA damage.
- Oxidizes unsaturated lipids such as squalene, sebaleic aicd, linoleic acid, and cholesterol. Activates lipoxygenase and cyclooxygenase.
- UV‑B 280-315 nm mostly absorbed by the ozone layer. Broad-spectrum sunscreen or sunblock blocks UV-A and UV-B.
- UV-C 180-280 nm completely absorbed by the ozone layer and atmosphere. Ionizing radiation causes pyrimidine dimers. Germicidal lamps are usually mercury-vapor lamps, which emit at 185 nm, blue, and green.
- The objective is a lens or mirror that gathers light.
- The aperture is the hole or an opening that allows light. The diaphragm or aperture stop blocks light. The entrance pupil is the front of the aperture.
- In the eye, the black pupil aperture is surrounded by the colored iris diaphragm.
- A pinhole camera is a small aperture that produces an inverted image.
- The rear focal point F’ is where parallel rays entering the system converge on the imaging plane. An ray from the front focal point F will emerge from the system parallel to the optical axis.
- The focal length f is the distance between the aperture and the focus. The eye has a 22 mm focal length. Longer focal length gives higher magnification and a narrower field of view.
- sin θ = r / f for pupil radius r and range of angles θ over which the system can accept light.
- f-number N = f / D.
- Numerical aperture (NA) = n sin θ. Index of refraction n is 1 in air.
- Rayleigh criterion: angular resolution = 0.61 λ / r. Resolution = angular resolution * f.
- Gaussian optics uses the paraxial approximation that rays make a small-angle to the optical axis and are close to the axis, so sin x = x.
- Abbe sine condition
- Aberrations cause blurring or distortion.
- spherical aberration
- chromatic aberration or color dispersion: convex lens has a higher magnification at blue than red. Causes blur and color fringing at high-contrast edges.
- Coma is a variation in magnification over the entrance pupil, so that off-axis point sources appear to have a tail (coma).
- Achromatic lens are corrected to bring red and blue into focus on the same plane, and corrects for spherical aberration at one wavelength. Commonly a doublet that combines a concave high-dispersion flint glass like F2 and convex (positive) low-dispersion crown glass like BK7.
- Apochromatic lens bring red, green, and blue into focus, and corrects for spherical aberration at two wavelengths.
- Fluorite or CaF2 has abnormal dispersion: a flat wavelength vs. refractive index plot. But hard to grow large crystals.
- Cardinal point
- The focal plane contains the focal point.
- The focus ring adjusts the focal point.
- Normal lenses are entocentric, with the pupil inside the lens.
- An object-space telecentric lens has its entrance pupil at infinity, providing an orthographic projection instead of a perspective projection.
- An image-space telecentric lens has its exit pupil at infinity, or a reversed object-space lens. It produces images of the same size regardless of the distance between the lens and the image sensor.
- A light field camera captures intensity and direction of light rays, allowing changing the focal distance. A hologram records a 3D wavefront on film.
- Wide-angle lens has a low focal length.
- Tilt-shift photography: tilt lens relative to the image plane to narrow the depth of field vertically.
- Bracketing or epsilon photography takes photos with a range of camera settings.
- Focus stacking combines images at multiple focal lengths to increase depth of field (DOF).
- High dynamic range (HDR) imaging uses exposure fusion.
- Image stitching combines the field of view from many images to produce a panorama.
- Strip photography captures a 1D image over time. Used in a photo finish.
- Ambiguity function represents distortion due to propagation delay and Doppler frequency of the receiver matched filter.
- Wavefront coding uses a phase modulating element and deconvolution to extend depth of field.
- A caustic is a curved envelope tangent to all its light rays. Refraction can create nephroids or cusps.
- https://en.wikipedia.org/wiki/Photographic_plate
- https://en.wikipedia.org/wiki/Orthochromasia#Orthochromatic_photography
Refraction
- Snell’s law of refraction: n sin theta is constant, where theta is the angle of incidence or angle of refraction, measured from the normal.
- refractive index measures how much light slows in a material, relative to vacuum.
- Causes total internal reflection for incidence angles (measured from the normal) greater than the critical angle.
- Dispersion occurs because blue light refracts at a larger angle than red light, so the refractive index varies with wavelength. Dispersion causes prisms, rainbows, and chromatic aberration.
Transverse waves oscillate perpendicular to the direction of motion, while longitudinal waves oscillate in the direction of motion.
Polarization is the direction of oscillation, determined by photon spin.
- Linear polarization is a fixed direction, while in circular oscillation the field rotates at a fixed rate.
- Birefringent materials have a refractive index that depends on the polarization of light, so unpolarized sources show a double refraction.
- Chiral materials have optical activity includes optical rotation and optical dichroism (differential absorption)
- Fresnel equations
An electromagnetic wave causes electrons in a material to oscillate proportional to the material’s magnetic susceptibility. This induces a phase-delayed wave of lower amplitude at same frequency. Phase 180 destructively interferes (light absorption). Phase 90 slows down the wave.
A rainbow is created when light from the sun enters a water droplet, reflects off the back, and passes back out of the droplet. Refraction causes the light to return at a 42° angle. Dispersion refracts blue light at a larger angle, and after the reflection, red light emerges at a larger angle, on the outside of the rainbow.
The antisolar point is the point on the celestial sphere directly opposite the sun.
A Brocken spectre is a midair shadow cast on fog. Depth perception is difficult, so the shadow can appear larger and further away that it really is.
Heiligenschein or hot spots are bright spots around a shadow in the presence of dew droplets, which act as lenses.
Rayleigh scattering (1971) is inelastic (energy-preserving) scattering due to polarizable molecules smaller than the wavelength of light. An electromagnetic wave causes the molecule to oscillate and radiate light. Blue light is scattered more than red light, so diffuse sky radiation is blue. In sunset, rays pass through up to 40 times more atmosphere, and blue light is scattered away. It scatters up to 0.1% of photons.
Raman scattering is elastic scattering, where a molecule gains vibrational energy from incident photons. It scatters ~1 ppm of photons.
Diffraction is a wave phenomenon. The classical Huygens–Fresnel principle states that every point on a wavefront is itself the source of spherical wavelets. For example, when a plane wave encounters a slit, it creates spherical ripples instead of a shadow. The small opening acts as a point source. For light, the source is a dipole, so waves are only emitted in the forward direction. The secondary waves can interfere with each other, producing bands of high and low amplitude. For light to exhibit wave properties, the slit should be comparable in size to the wavelength.
The double-slit experiment demonstrates wave–particle duality. A source can emit single photons or even electrons which are clearly detectable as individual particles hitting a screen. But the spatial bands still show wave interference.
- https://www.youtube.com/watch?v=dtcq5b0R65w
- The Mach–Zehnder interferometer is a simpler double path setup.
- Kirchhoff’s diffraction formula
- Fresnel diffraction in near field (close to the object)
- Fraunhofer diffraction in far field
A diffraction grating disperses light in different angles depending on wavelength. It can be reflective using ridges or transmissive using slits.
Structural colors are produced by wave interference on a microscopic structure.
Iridescence is a change in color based on angle.
The Airy disc is the diffraction blur of a point source.
The Arago spot is a faint spot of light at the center of a circular object’s shadow.
Thin-film interference are colorful patterns on soap bubbles and oil films due to interference between light waves reflected from the top and bottom surface of the film. Newton’s rings are patterns on a curved glass touching a flat surface due to interference between reflections.
Fluorescence: emit light at a different wavelength. Antifreeze contains fluorescein to detect radiator leaks.
Phosphorescence: emit light at a later time, usually at a longer wavelength.
Optical fiber: core has a higher refractive index than the cladding.
Optical pumping: add photons with the exact transition energy, achieving population inversion.
- Drives laser stimulated emission.
- Measures Zeeman effect: change in energy levels due to a magnetic field.
- Prepares energy levels in atomic clocks.
Optical module is an optical transceiver between electrical systems and fiber optic cables.
- A coherent optical module uses coherent modulation (BPSK/QPSK/QAM) rather than amplitude modulation (RZ/NRZ/PAM4).
- Pulse Position Modulation (PPM) uses photon-counting detectors. At room temperature, infrared or higher frequencies are needed to surpass thermal Johnson-Nyquist noise. They have a Poisson noise distribution which leads to the Gordon-Holevo limit.
Optical amplifier: pump laser achieves population inversion. Signal light can stimulate excited atoms in the doped core to emit a photon at the same wavelength, which cascades.
- core pumping directly excites the dopant ions, but requires coupling the pump laser into the core, which can have some losses.
- cladding pumping excites the core through evanescent coupling. In evanescent coupling, the reflected wave extend into the interface by a few wavelengths, decaying exponentially with distance.
- erbium-doped fiber amplifier (EDFA) is the most common.
An optical circulator is a passive non-reciprocal device, where light entering one port exits the next port with low loss (1 dB) and high isolation (20 dB) of the other direction.
- Often uses a Faraday rotator using a magnetic field to rotate the plane of polarization.
- Allows bi-directional communication over a single fiber.
- Filters pump light in amplifiers and backscattered light in sensors.
- Add-Drop Multiplexers (ADM) extract a specific wavelength division multiplexing (WDM) channel.
https://en.wikipedia.org/wiki/Dichroism
https://en.wikipedia.org/wiki/Pleochroism
X-rated ptychography requires high energy x-rays.
The dress (2015) is a viral phenomenon about unusually large differences in perceived color. The photo of a blue and black dress under yellow illumination can also be interpreted as a white and gold dress under blue illumination.
https://en.wikipedia.org/wiki/The_dress#See_also
Lateral inhibition of neurons
The spectral power distribution is the radiant exitance by wavelength.
Photopic vision occurs in well-lit conditions (10 to 10^8 cd/m^2) via cone cells, which have peak absorption at 420 nm (blue), 534 nm (bluish green), and 564 nm (yellowish green). Color vision is limited to 400 to 700 nm.
Scotopic vision is vision in dark conditions. Rod cells are most sensitive to 498 nm wavelength.
A Lambertian reflector is an ideal matte surface, with reflected radiance the same in all directions, following Lambert’s cosine law: radiant intensity is proportional to the cosine between the observer’s line of sight and the surface normal.
Color
- An illuminant is defined by its spectral power distribution.
- Color space is 3D.
- Chromaticity is the hue and colorfulness or saturation of a color.
- Luma is the objective or linear light brightness. Luminance are its log values or gamma-corrected values in nonlinear space.
- Black body radiation such as incandescent light is determined by its temperature per Planck’s law: 1700 K is warm, 5500 K is daylight, and 15000 K is blue sky. Red heat changes from red to yellow to white. The Planckian locus is the line of possible black body colors in a chromaticity space.
- The correlated color temperature of a light is the black body temperature with the closest perceived color. Fluorescent lights tend to be more green. The color rendering index (CRI) measures how close a spectrum resembles daylight, with a maximum of 100.
- White point is the appearance of a white object under a light source. Color correction corrects orthogonal to the Planckian locus, on a green-magenta axis.
A staring array uses an array of sensing pixels. A push broom scanner or along-track scanner sweeps a scan line. A whisk broom scanner or across-track scanner sweeps a single detector in 2D.
Projection of an object onto the projection plane or image plane
- Linear perspective: lines of sight or rays converge
- Ground line
- Station point on the true-height line
- 1-point: vanishing point on the horizon line.
- 2-point: vanishing points on the horizon line.
- 3-point: third point on the true-height line.
- Parallel perspective: parallel rays
- orthographic projection: rays perpendicular to the image plane
- Isometric: three coordinate axes are equally foreshortened and at 120 angles.
- Oblique projection: rays at a skew angle
Relativity
Special relativity is the theory of spacetime. It postulates that the speed of light in vacuum is the same for all observers, and that the laws of physics are invariant in all inertial frames of reference. It predicts mass-energy equivalence, E = mc^2. It is the an approximation of general relativity for flat spacetime or Minkowski space.
In Minkowski space, an event is described by the 4-position (ct, x, y, z). The speed of light converts time units to space units. The metric tensor is 1 0 / 0 -I_3 (metric signature +—).
The spacetime interval is invariant in all coordinate frames, whereas time intervals and lengths are not. Intervals traveled by light are lightlike, with s^2 = 0. Intervals traveled by massive objects are timelike: s^2 > 0. Spacelike intervals have s^2 < 0. The light cone at a given point defines timelike past (causal influences), timelike future (causal effects), and spacelike (causally unrelated events). Simultaneity is relative for spacelike-separated events.
The proper time interval, elapsed time as measured for a clock following the line, is invariant for timelike world lines.
The Lorentz transformation transforms spacetime coordinates between inertial frames with different relative velocities, explaining length contraction and time dilation.
A particle with 3-position r(t) and 3-velocity u = dr/dt has Lorentz factor γ(u) = 1/sqrt(1 - |u|2/c2).
In the instantaneous rest frame where the particle is always at rest, we have dr = 0 and ds^2 = c^2 d𝜏^2. For another frame, we have ds^2 = ct^2 - dr^2. Thus the time dilation is dt = γ(u) d𝜏.
The four-velocity U = dX/d𝜏 = dX/dt dt/d𝜏 = γ(u)(c, u), and the magnitude |U| = c.
The four-momentum P = m_0 U = m_0 γ(u)(c, u) = (E/c, p) for rest mass m_0. We have |P|^2 = m_0^2 c^2 = (E/c)^2 + |p|^2. The energy–momentum relation E^2 = (pc)^2 + (m_0 c2)2 decomposes energy into momentum and rest mass.
Geometrized units set c = 1, dimensionless, making time and length equivalent. Mass is the magnitude of the four-momentum vector, so it must have units of length, so the gravitational constant G = 1. The Schwarzschild radius of a black hole with mass m becomes r = 2m.
Cosmological constant problem. The theoretical zero-point energy from vacuum fluctuations of matter fields and force fields is 1e60 higher than the vacuum energy density implied by the observed cosmological constant.
General relativity is the theory of gravitation. The curvature of spacetime is related to the stress–energy tensor representing the density of energy and momentum. Spacetime curves with matter, propagates waves, bends light, etc.
- 1967 Wheeler–DeWitt equation of quantum gravity.
Lorentzian manifold.
A metric tensor is a bilinear form. It gives infinitesimal distance on a manifold, and allows computing distances on the manifold by integration.
- The Euclidean metric for (x, y) coordinates is I_n, so ds^2 = dx^2 + dy^2 for line element ds.
The Einstein field equations are G_{μν} + Λ g_{μν} = κ T_{μν}.
- the Einstein tensor G_{μν} is the spacetime curvature.
- the metric tensor g_{μν}(x,y,z,t) is the geometric and causal structure of spacetime, which has energy carried by gravitons.
- the stress–energy-momentum tensor T_{μν} is the distribution of energy and matter
- cosmological constant Λ
- the Einstein gravitational constant κ = 8πG/c^4
This metric reduces to Newton’s law of gravitation for non-relativistic velocities and masses. Q: why?
FRW metric (Friedmann–Lemaître–Robertson–Walker or FLRW).
-c^2 d𝜏^2 = -c^2 dt^2 + a(t) dΣ^2
Σ ranges over a 3D space of uniform curvature, and a(t) is the cosmic scale factor that characterizes the expansion of the universe.
ΛCDM (lambda cold dark matter) is the standard model of Big Bang cosmology based on general relativity.
The Hubble constant H = a’/a.
For a Λ-dominated universe, the Friedman equations state that H = H_0 * sqrt(Ω) is a constant, which implies exponential growth.
Consider a perfect fluid described by scalar field ϕ with time derivative ϕ’, pressure P, energy density ρ, potential energy V(ϕ), and four-velocity u_μ.
The energy-momentum tensor is T_{μν}=(ρ+P)u_μ u_ν +Pg_{μν}.
Equation of state parameter w = P / ρ = (1/2 ϕ’^2 - V(ϕ)) / (1/2 ϕ’^2 + V(ϕ)). Positive vacuum energy implies w = -1 and negative pressure.
https://en.wikipedia.org/wiki/Wilkinson_Microwave_Anisotropy_Probe
Quantum mechanics
Quantum states have unit 2-norm. (In contrast, classical probabilities sum to 1 or have unit 1-norm.) A binary state or qubit (a, b) has outcomes with P(0) = a^2 and P(1) = b^2. In Dirac notation, a qubit is a|0> + b|1>, where a is the amplitude of outcome |0>. Stochastic matrices contain columns of nonnegative real numbers that sum to 1. For example, a bit flip is ((0 1) (1 0)).
Negative amplitudes enable quantum interference. Consider the counterclockwise 45 degree rotation matrix ((1/√2 -1/√2) (1/√2 1/√2)). Rotating the state |0> leads to an entangled state, but rotating again causes destructive intereference between the paths to |0>.
Operations are unitary matrices. Amplitudes can be complex numbers so that every unitary operation, such as the mirror transfrom ((1 0) (0 -1)), has a square root.
A wave function \(|\phi\rangle\) represents a quantum state at a fixed time. \(\phi\) maps its domain (e.g. position) to probability amplitudes (complex numbers). The wave function represents a vector in the state space H, the complex Hilbert space over wave functions.
Q: why do we need probability amplitudes?
Born rule. The probability of an observation is proportional to the square of the amplitude of the wavefunction (projection onto the corresponding eigenvector). This implies that \(E[A] = \phi \dot A\phi\). They can be normalized to unit L2 norm and are generally restricted to be square-integrable (L2 norm exists). Operators are unitary, satisfying \(U^*U=UU^*=I\), the complex analogue of an orthogonal matrix which preserves vector norms.
A metric space M is complete if every Cauchy sequence in M has a limit that is also in M (there are “no points missing”).
A Hilbert space H is a vector space that is also a complete metric space with the induced distance function. For a complex Hilbert space, the inner product is conjugate symmetric (aka Hermitian symmetric): \(<y, x> = \overline{<x, y>}\).
A Banach space is a space that is complete under the metric induced by a norm. A Hilbert space is an inner product space that is a Banach space.
An observation collapses the state space so that only outcomes consistent with the observation are possible. The new state is the projection onto the eigensubspace associated with the observation.
An observable represents a measurable physical quantity. The possible result are its eigenvalues. Real-valued eigenvalues imply that an observable is a self-adjoint operator, or a Hermitian matrix in finite dimensions. A Hermitian matrix is equal to its conjugate transpose, the complex analog of a symmetric matrice. More generally, a self-adjoint operator is a linear endomorphism that is its own adjoint. The Hermitian adjoint operator A* generalizes the conjugate transpose of a matrix and is defined as \(\langle Ax,y \rangle = \langle x,A^*y \rangle\).
https://en.wikipedia.org/wiki/Bra%E2%80%93ket_notation
Conjugate variables are Fourier transform duals.
Noether’s theorem states that a symmetry with respect to one conjugate variable implies that the other conjugate variable will not change with time (i.e. it will be conserved).
A Fourier transform maps wave functions over position to wave functions over momentum. (Pontryagin duality)
Complementary properties cannot be measured simultaneously because their observables are incompatible or fail to commute.
The Heisenberg uncertainty principle states that
\(\sigma_x\sigma_p\geq {\frac{\hbar}2}\). For a general operator, \(\sigma_O = \sqrt{E[O^2] - E[O]^2}\) and the commutator is \([A, B] = AB - BA\), and \(\sigma_A\sigma_B \geq \left|\frac1{2i} \langle [A, B]\rangle\right|\).
Quantum entanglement.
- The principle of locality says that things can only be influenced by their immediate surroundings, and interactions can’t travel faster than light.
- Bell’s theorem or the Bell inequality shows that measurements on one entangled particle instantly affects the other. It rules out local hidden-variable theories, which used hidden variables (nonmeasurable properties of particles) to explain quatum phenomena.
- Quantum eraser: run a double-slit experiment with entangled photons. Measuring one photon erases the interference pattern of its entangled photon.
Canonical commutation relation. For any conjugate variables \(x\), \(p\), the commutator \([x, p] = i\hbar I\).
\(i\hbar {\frac {d}{dt}}|\psi (t)\rangle =H(t)|\psi (t)\rangle\). The time derivative of a quantum state is \(-i/\hbar H\).
The Schrödinger equation gives the evolution over time as a unitary transformation on the initial state: \({|\psi (t)\rangle =U(t;t_{0})|\psi (t_{0})\rangle }\).
- https://en.wikipedia.org/wiki/Schr%C3%B6dinger%27s_cat
Electrons have intrinsic angular momentum, which affects how they are deflected by a strong magnetic field. The Pauli equation describes how spin 1/2 particles interact with an external electromagnetic field. It is the non-relativistic approximation of the Dirac equation.
Harmonic oscillator, hydrogen atom.
The Hamiltonian operator is the observable corresponding to the total energy of that system. The energy spectrum is the set of possible outcomes obtainable from a measurement of the system’s total energy.
For a single particle of mass \(m\), H = T + V for potential energy V and kinetic energy $T = $.
The momentum operator \(p =-i\hbar \nabla\), and kinetic energy \(T = p^2 / 2m\).
The Planck constant \(h\) is the product of the wavelength lambda of a particle and its momentum p.
For a photon, E = hf. The reduced Planck constant \(\hbar = h/2\pi\) relates energy to angular frequency (radians per second), explaining the photoelectric effect.
Matter waves are also known as de Broglie waves. Momentum \(p = \hbar k\), where k is the wave vector in inverse meters.
Fermi energy is the difference between the highest and lowest occupied single-particle states in a quantum system.
- The real lattice of a crystal is the periodic physical arrangement of atoms. Covariant.
- The reciprocal space or k space is the Fourier transform of the real lattice, in a space of spatial frequencies k. Contravariant.
- Momentum space: momentum p = ℏk.
- The Fermi surface is the surface in reciprocal space which separates occupied from unoccupied electron states.
- Fermi temperature = Fermi energy / Boltzmann constant. Temperature at which thermal effects are comparable to quantum effects. Much higher than room temperature.
- Fermi momentum = \(\sqrt{2 m E}\) and Fermi velocity describe velocity at the Fermi surface.
Particle in a box model: in classical systems, a particle can move at any speed, whereas at nm scale, particle energy levels are discretized and it can never have zero energy level.
- Spatial nodes: positions where the particle can never be.
Quantum harmonic oscillator
Quantum numbers are conserved quantities that can be measured together as eigenvalues of operators that commute with the Hamiltonian.
- An electron in an atom has principal quantum number (n), its electron shell or energy level; azimuthal quantum number (ℓ), the subshell s, p, d, or f; magnetic quantum number (mℓ), the specific orbital in the subshell; and spin quantum number (ms), the spin angular momentum by its circulating flow of charge.
https://en.wikipedia.org/wiki/Wave_packet
https://en.wikipedia.org/wiki/Particle_in_a_box
https://en.wikipedia.org/wiki/Quantum_harmonic_oscillator
https://en.wikipedia.org/wiki/Quantum_uncertainty
https://en.wikipedia.org/wiki/Interpretations_of_quantum_mechanics
https://en.wikipedia.org/wiki/Copenhagen_interpretation
https://en.wikipedia.org/wiki/Wave_function_collapse
https://en.wikipedia.org/wiki/Template:Quantum_mechanics_topics
Quantum information theory
Particle physics
Quantum field theory (QFT) treats particles as excited states of their underlying quantum fields. Particle motion is described by minimizing the action of the Lagragian, a functional of the particle field.
A gauge theory is a field theory where the Lagriangian (the system dynamics) is gauge invariant under local symmetry transformations. The symmetry group (Lie group or gauge group) forms a Lie algebra of group generators. Each group generator produces a gauge field. An abelian gauge theory has a commutative symmetry group.
In the fiber bundle formulation, a gauge theory studies parallel transport connections on vector bundles, principal bundles, and fibre bundles. The theory associates a fiber, a copy of the gauage group G, at each point in spacetime. A fiber bundle is a space that is locally a product space R^d x G, but can have some global twisted topology. A loop representation is in the space of Gauss gauge invariant physical states, avoiding the redundancy of Gauss gauge symmetries.
A Wilson loop W[γ]
is a gauge invariant operator arising from the parallel transport of a gauge variable around a closed loop. It is an order operator whose expectation characterizes phase transitions. It is defined as the trace of closed Wilson lines. The confining phase is described by the loop in spacetime traced out by a quark–antiquark pair created at one point and annihilated at another point. The action of the loop E[W[γ]]
follows the area law. In the nonconfining Higgs phase, the expectation follows the perimeter law.
The S-matrix or scattering matrix is the unitary matrix connecting sets of asymptotically free particle states.
https://news.ycombinator.com/item?id=40456801
A special unitary group is the Lie group of unitary matrices with determinant 1.
The three Pauli matrices is the observable representing spin in the three spatial dimensions. They are unitary, with eigenvalues 1 and -1. They span the Lie algebra of the SU(2) group.
The eight Gell-Mann matrices span the Lie algebra of the SU(3) group.
https://en.wikipedia.org/wiki/Exponential_map_(Lie_theory)
The Standard Model describes the electromagnetic, weak, and strong interactions. It classifies all known elementary particles into bosons and fermions.
Bosons are the quantized exchange interactions or force carriers for gauge fields: photon (EM), W and Z bosons (weak), eight gluons (strong), and the scalar Higgs boson. They have integer spin and obey Bose–Einstein statistics.
Fermions include quarks and leptons. Fermions have half-integer spin and obey the Pauli exclusion principle and Fermi–Dirac statistics.
Symmetrization postulate: the wavefunction in 3D of a system of identical particles is either totally symmetric (bosons) or totally antisymmetric (fermions) when exchanging two particles. It implies the Pauli exclusion principle that two fermions cannot share the same set of quantum numbers.
https://en.wikipedia.org/wiki/Mathematical_formulation_of_the_Standard_Model
Quantum electrodynamics (QED) is an abelian gauge theory with symmetry group U(1) and the electromagnetic four-potential gauge field quantized as the photon. Theory of wave-particle duality.
Yang-Mills theory is the field theory of special unitary groups.
The weak force SU(2) has three force carriers: W and Z bosons, where W bosons have spin 1 and -1. There are two types of interactions, where current refers to the exchange of the boson.
W bosons mediate charged current interactions. Weak isospin is a 3D vector T with T_3 being important. It is conserved in electroweak and strong interactions. Higgs interactions do not conserve weak isospin but does conserve charge Q = T_3 + 1/2 Y_W. Weak hypercharge Y_W corresponds to the gauge symmetry U(1).
- Beta decay
- Neutron -> proton + e- + antineutrino
- Positron emission or β+ decay: proton -> neutron + e+ + ν_e. In the neutron, d -> u + W-, and \(W- \rightarrow e- + \bar{\nu_e}\).
- \(\mu^- + W^+ \rightarrow \nu_\mu\): a muon changes to a muon neutrino by absorbing a W+ boson.
The Z boson mediates neutral current interactions. The weak charge Q_w quantifies the force of the interaction. e- -> e- + Z, and \(Z \rightarrow b + \overline{b}\): an electron emits a Z boson, which decays rapidly.
Weak isospin describes interaction with W bosons; color charge for gluons (strong force).
https://en.wikipedia.org/wiki/Weak_isospin
The Higgs field is the only scalar field with two neutral and two electrically charged components. It is nonzero everywhere, breaking the weak isospin SU(2) symmetry. The Higgs mechanism is responsible for all rest masses in the Standard Model.
Leptons are fermions that do not undergo strong interactions. They can be charged or neutral: (1) electron and electron neutrino ν_e, (2) muon and muon neutrino, and (3) tauon and tauon neutrino. Neutrino oscillation implies that the neutrino has mass. The Koide formula is an intriguing empiral relation between the masses for the three generations. The Deep Underground Neutrino Experiment (DUNE) at Fermilab studies proton decay.
Quantum chromodynamics (QCD) is the nonabelian gauge theory SU(3) of the strong force, which acts on quarks through gluons. Isospin is a symmetry of the strong interaction under the action of SU(2). The isospin operator is vector-valued. I_3 is the eigenvalue of the I_Z projection, which is a Pauli matrix 1/2 𝜏_3.
Gluons come in eight types, identifiable by superpositions of color-anticolor states. The color singlet state (equal probability of all three color-same anticolor states) is excluded. Thus there are eight possible types. In asymptotic freedom, the strong force decreases at high energies and short distances, so that quarks can move freely inside protons.
Quarks have charge +2/3 or -1/3, and come in three generations: (1) up and down, (2) charm and strange, (3) top and bottom. Up and down quarks have isospin +1/2 and -1/2. Heavier generations have isospin 0 and are more rare. Quarks also have color charge (rbg), which ensures color confinement. The gluon field between a quark and antiquark forms a flux tube or string between them with constant force (10 kN), and the work required to separate them quickly exceeds the energy need for a new quark-antiquark pair to appear.
Hadrons are composite particles made up of quarks bound by the strong force. Baryons are fermions with an odd number of quarks, mainly three quarks of different colors. E.g. protons (uud) and neutrons (udd). Mesons are bosons with quarks paired in singlets, mostly pions (quark and antiquark).
CPT symmetry. Any Lorentz invariant local quantum field theory with a Hermitian Hamiltonian.
- C-symmetry (charge symmetry), a universe where every particle is replaced with its antiparticle
- P-symmetry (parity symmetry), a universe where everything is mirrored along the three physical axes
- The Wu experiment shows that weak interactions do not conserve parity.
- The Fitch–Cronin experiment in 1964 observes CP violation.
- T-symmetry (time reversal symmetry)
It does not fully explain baryon asymmetry (matter–antimatter asymmetry).
Photoelectric effect: quantized photon energy proportional to frequency. Can also emit photons: photoluminescence.
Black-body radiation. Quantization is needed to explain why the ultraviolet catastrophe does not happen–why there is not unbounded radiation at high frequencies. The equipartition theorem in classical statistical mechanics states that each degree of freedom (frequency) has an average energy of k_B T. But the number of harmonic oscillator modes per frequency increases unboundedly.
The mass number A is the sum of atomic number (proton number) Z and neutron number N.
- Isobars are atoms with the same number of nucleons (protons or neutrons).
- The nuclear force is the residual strong force between two neutrons and/or protons. It is carried by hadrons and has range around 1 fm.
- The nuclear binding energy is the mass defect of a nucleus: the total free mass of its constituent protons and neutrons minus its actual mass.
- Iron is the most stable nucleus. Lighter elements can fuse, and elements heavier than lead can undergo alpha decay.
- The isobar with the highest nuclear binding energy is most stable.
- Semi-empirical mass formula (SEMF) estimates Z from proton and neutron count.
- The valley of stability starts at roughly Z = N (proton-neutron ratio = 1) and curves slightly to require Z > N for large nuclei.
- Beta-decay stable isobars cannot undergo beta decay.
- Island of stability: predicted set of superheavy isotopes around the predicted closed neutron shell N = 184.
- Alpha decay ejects a helium nucleus (two protons and two neutrons) typically with 5 MeV of energy or 4% of c. It has low penetration (an inch of air) and is highly ionizing.
- Nuclear shell model. Maria Goeppert Mayer and J. Hans D. Jensen, half of the 1963 Nobel Prize.
- Nucleons have distinct quantum numbers by the Pauli exclusion principle. They fill shells from the lowest energy level.
- Proton and neutron shells are independent.
- Atomic nuclei with a magic number of nucleons are much more stable because they form a filled shell.
- helium, oxygen, calcium, nickel, tin, lead (2, 8, 20, 28, 50, 82).
Condensed matter physics
Superfluids can flow without energy dissipation.
Superconductors have zero resistance below a critical temperature Tc.
- Superfluid of bound Cooper pairs of electrons. It can flow without energy dissipation because the energy gap needed to excite the Cooper pairs is larger than the thermal energy kT of the lattice.
- Persistent electric current flows.
- Above the critical temperature, thermal vibrations break the Cooper pairs.
- 1933. Meissner effect: expulsion of magnetic field from a superconductor, which will repel a nearby magnet. By conservation, the exterior magnetic flux increases.
- 1935. London equations relate superconducting current to electromagnetic fields.
- London penetration depth λ: distance to which a magnetic field penetrates into a superconductor.
- Type-I superconductors break down abruptly as the external magnetic field exceeds the critical value. Pure metals, and tantalum silicide and boron-doped silicon carbide SiC:B.
- Type-II superconductors have a mixed state with increasing magnetic penetration but still zero electric current, due to quantized vortices or fluxons in the electronic superfluid. Niobium, carbon nanotubes, and compound semiconductors.
- https://en.wikipedia.org/wiki/Template:Superconductivity
The thermal de Broglie wavelength is the average de Broglie wavelength of particles in an ideal gas at a given temperature. When particles are usually closer than this distance, the gas must be treated as a Fermi gas or a Bose gas: Bose–Einstein statistics or Fermi–Dirac statistics. When particles are further apart, they can obey Maxwell–Boltzmann statistics.
- A Fermi gas consists of many noninteracting fermions.
Ionization produces an ion pair: an electron and a positive ion.
A Townsend avalanche is a cascade of gas ionization. An electric field accelerates each freed electron to free additional electrons.
A gaseous ionization chamber has an electric field to prevent ion pairs from recombining. It uses a cylinder with a coaxial anode wire or parallel plates. It lasts longer in high radiation fields.
A proportional counter measures the energy of ionizing particles to determine absorbed dose or distinguish between alpha and beta particles. A medium electric field creates an ion drift region, where the number of ion pairs is proportional to the energy of the ionizing particle. A 1 MeV particle can create about 30,000 ion pairs. Near the anode wire (<1 mm), the field is strong enough to amplify signal through localized avalanches.
A wire chamber uses a grid of wires acting as proportional counters. A micropattern gaseous detector (MPGD) has a sub-millimeter grid. The MicroMegas detector (1992) has a gain of 10,000. A gas electron multiplier consists of a thin polymer sheet layered with copper on both sides, with a voltage difference. Photolithography creates uniform small holes, and a single ion entering a hole can emit up to 1,000 electrons. A triple stack can result in a gain over 1 million.
A cloud chamber is saturated with water vapor. A charged particle traces a track of ionized gas particles, which form condensation centers. A magnetic field results in a radius of curvature of a charged particle proportional to its momentum.
A bubble chamber is filled with superheated liquid. A charged particle creates ions surrounded by vapor, and decreasing the pressure grows the bubbles to visible size.
Compton scattering. A high-frequency photon releases electrons from an atom.
https://en.wikipedia.org/wiki/Cherenkov_radiation
Second: Caesium standard
https://en.wikipedia.org/wiki/LIGO
https://en.wikipedia.org/wiki/Black_hole_thermodynamics
https://en.wikipedia.org/wiki/Holographic_principle
https://en.wikipedia.org/wiki/Bogomol%27nyi–Prasad–Sommerfield_bound
String theory
https://en.wikipedia.org/wiki/History_of_string_theory
https://en.wikipedia.org/wiki/M-theory
https://en.wikipedia.org/wiki/AdS/CFT_correspondence
https://en.wikipedia.org/wiki/Template:Breakthrough_of_the_Year
A particle acclerator accelerates charged particles to relativistic speeds.
- A linear particle accelerator generate X-rays or high energy electrons via oscillating fields.
- A cyclotron accelerates particles in a spiral trajectory.
- A synchrotron synchronizes the magnetic field to the particle energy, allowing the highest energies.
- The Relativistic Heavy Ion Collider is first heavy-ion collider.
- The Swiss Light Source produces bright hard X-rays, including for protein crystallography.
Nuclear power plants
The Large Hadron Collider LHC can accelerate protons to 7 TeV in a 17 mi circumference ring.
https://en.wikipedia.org/wiki/COMPASS_experiment
https://en.wikipedia.org/wiki/Super_Proton_Synchrotron
CMS
ATLAS
ALICE
LHCb
A tokamak confines plasma in a toroidal chamber with magnetic coils.
https://en.wikipedia.org/wiki/Template:Beyond_the_Standard_Model
- Grand Unified Theory (GUT) merges the gauge interactions (electroweak and strong interactions) into one electronuclear interaction at high energies or in the grand unification epoch in the very early universe.
- Single coupling constant, which determines the strength of a force.
- Theory of everything (TOE) fully explains the universe, merging small-scale quantum mechanics and large-scale general relativity (gravity)
- Planck scale: quantum effects of gravity become significant at the Planck energy, 10e28 eV
Nuclear reactors have become safer, more modular, with less waste, and more fuel efficient.
- Light-water reactor (LWR): reactor vessel uses normal water as its coolant and neutron moderator. Most common type. After driving the turbines, the steam is condensed back into water. External water is needed to cool the condenser.
- Reactor core can raise or lower rods.
- nuclear fuel rods, 12’ long, pencil thin, uranium oxide
- control rods: hafnium or cadmium absorb neutrons.
- Boiling water reactor (BWR): fission heat turns water into steam, which drives turbines. Fewer large steam supply components.
- Pressurised water reactor (PWR): fission heat is transferred to a secondary loop which contains the turbines. Water is kept under pressure to avoid boiling and forming steam bubbles.
- Heavy-water reactor (HWR) uses D2O as its coolant and neutron moderator. Heavy water is expensive to isolate, but it has lower neutron absorption, increasing neutron economy and allowing natural uranium instead of enriched fuel.
- Emergency core cooling system (ECCS)
- High pressure coolant injection (HPCI)
- Automatic depressurization system (ADS) enables high-capacity LPCI systems.
- 1950. Generation I: water-cooled, research-only.
- 1970. Generation II
- A breeder reactor breeds more fuel than it consumes.
- A fast-neutron reactor (FNR) breeder sustains the fissile chain reaction using fast neutrons above 1 MeV. It needs fuel relatively rich in fissile material. Produces no transuranic waste.
- Sodium-cooled fast reactor. Sodium has a high boiling point and does not need pressurization, allowing a thinner vessel which can be passively cooled. It also has a high heat capacity and is not corrosive.
- 1995. Monju accident: sodium leak caused a fire.
- Zirconium alloy cladding prevents contamination of reactor coolant. It is corrosion resistant with low neutron absorption.
- Mixed oxide (MOX) fuel (uranium oxide and plutonium oxide), axial shuffling, and radial zoning improve fuel burn-up.
- 1990. Generation III: passive safety systems include convection cooling without need for pumps. EPR and AP1000.
- Fourth generation
- Molten salt reactors
- Advanced boiling water reactor (ABWR): reactor internal pumps reduce piping needs.
- 1979. Three Mile Island.
- Condensate polisher uses resins to remove ions from condensed water, protecting downstream generators.
- Increasing water pressure to clear the resin filter sent water into an air line, shutting down the steam turbines. Heat increased, shutting down the reactor and opening the reactor pilot-operated relief valve (PORV). Emergency feedwater lines were closed, leading to a loss of coolant accident (LOCA) and melting half the fuel. Instrument design flaws caused delays in identifying the problem.
- 1986. Chernobyl disaster: accumulation of the neutron absorber xenon-135 and human error led to very low power output. Operators removed too many control rods to increase power output, while increasing coolant flow rate.
- Gen II graphite-moderated RBMK.
- Inserting control rods caused an initial power spike by displacing neutron-absorbing water with graphite, a neutron moderator. At maximum extraction, the graphite section was centered with 4’ columns of water above and below.
- Large positive void coefficient: formation of steam bubbles from boiling coolant reduced neutron absorption, leading to meltdown.
- 2011. Fukushima nuclear accident, 0 killed. Tsunami flooded seawater pumps, leading to loss of coolant accident (LOCA), melted fuel, and hydrogen explosions from steam-zirconium reactions. The AC emergency diesel generators (EDG), the DC batteries, and crucial power distribution buses were also damaged, and the control room lost lights, monitoring, and control. The plant was not designed for severe tsunamis. Emergency pumps were at low ground without waterproofing or adequate seawalls.
Fusion power
- 1955. Lawson criterion: net power = efficiency * (fusion - radiation loss - conduction loss).
- The triple product of density, confinement time, and plasma temperature T may be more useful.
- fusion = fuel number density * fusion cross section * energy per reaction
- cross section or P(fusion event) depends on plasma temperature
- Need temperatures around 100 million kelvin.
- A breeding blanket produces tritium fuel.
- Inertial confinement fusion (ICF) by laser.
- National Ignition Facility (NIF) laser
- 1985. Z Pulsed Power Facility is the largest electromagnetic wave generator.
- magnetic confinement fusion (MCF)
- Tokamak like ITER
- Earlier systems
- Z-pinch
- Stellarotor
- Magnetic mirror