Misplaced Pages

JEDI

Article snapshot taken from Wikipedia with creative commons attribution-sharealike license. Give it a read and then ask your questions in the chat. We can research this topic together.

JEDI ( Jupiter Energetic-particle Detector Instrument ) is an instrument on the Juno spacecraft orbiting planet Jupiter . JEDI coordinates with the several other space physics instruments on the Juno spacecraft to characterize and understand the space environment of Jupiter's polar regions, and specifically to understand the generation of Jupiter's powerful aurora. It is part of a suite of instruments to study the magnetosphere of Jupiter . JEDI consists of three identical detectors that use microchannel plates and foil layers to detect the energy, angle, and types of ion within a certain range. It can detect electrons between 40 and 500 keV (Kilo electron-volts), and hydrogen and oxygen from a few tens of keV to less than 1000 keV (1 MeV). JEDI uses radiation-hardened Application Specific Integrated Circuits (ASIC)s. JEDI was turned on in January 2016 while still en route to Jupiter, to study interplanetary space. JEDI uses solid state detectors (SSDs) to measure the total energy ( E ) of both the ions and the electrons. The MCP anodes and the SSD arrays are configured to determine the directions of arrivals of the incoming charged particles. The instruments also use fast triple coincidence and optimum shielding to suppress penetrating background radiation and incoming UV foreground.

#458541

38-411: JEDI is designed to collect data on "energy, spectra, mass species (H, He, O, S), and angular distributions"; the plan is to study the energies and distribution of charged particles. It can detect them at between 30  keV and 1 GeV, whereas JADE , another instrument on the spacecraft, is designed to observe below 30 keV. One of the concepts being studied is how energy from Jupiter's rotation

76-483: A gas or plasma then the time-scales for atom-atom interactions are huge in comparison to the atomic processes that are generally considered. This means that the individual atoms can be treated as if each were in isolation, as the vast majority of the time they are. By this consideration, atomic physics provides the underlying theory in plasma physics and atmospheric physics , even though both deal with very large numbers of atoms. Electrons form notional shells around

114-455: A positron , each with a mass of 0.511 MeV/ c , can annihilate to yield 1.022 MeV of energy. A proton has a mass of 0.938 GeV/ c . In general, the masses of all hadrons are of the order of 1 GeV/ c , which makes the GeV/ c a convenient unit of mass for particle physics: The atomic mass constant ( m u ), one twelfth of the mass a carbon-12 atom, is close to

152-461: A neutral atom, the system will emit a photon of the difference in energy, since energy is conserved. If an inner electron has absorbed more than the binding energy (so that the atom ionizes), then a more outer electron may undergo a transition to fill the inner orbital. In this case, a visible photon or a characteristic X-ray is emitted, or a phenomenon known as the Auger effect may take place, where

190-491: A photon are related by E = h ν = h c λ = 4.135   667   696 × 10 − 15 e V / H z × 299 792 458 m / s λ {\displaystyle E=h\nu ={\frac {hc}{\lambda }}={\frac {\mathrm {4.135\ 667\ 696\times 10^{-15}\;eV/Hz} \times \mathrm {299\,792\,458\;m/s} }{\lambda }}} where h

228-442: A single nucleus that may be surrounded by one or more bound electrons. It is not concerned with the formation of molecules (although much of the physics is identical), nor does it examine atoms in a solid state as condensed matter . It is concerned with processes such as ionization and excitation by photons or collisions with atomic particles. While modelling atoms in isolation may not seem realistic, if one considers atoms in

266-413: A system of natural units in which the speed of light in vacuum c and the reduced Planck constant ħ are dimensionless and equal to unity is widely used: c = ħ = 1 . In these units, both distances and times are expressed in inverse energy units (while energy and mass are expressed in the same units, see mass–energy equivalence ). In particular, particle scattering lengths are often presented using

304-686: A unit of inverse particle mass. Outside this system of units, the conversion factors between electronvolt, second, and nanometer are the following: ℏ = 1.054   571   817   646 × 10 − 34   J ⋅ s = 6.582   119   569   509 × 10 − 16   e V ⋅ s . {\displaystyle \hbar =1.054\ 571\ 817\ 646\times 10^{-34}\ \mathrm {J{\cdot }s} =6.582\ 119\ 569\ 509\times 10^{-16}\ \mathrm {eV{\cdot }s} .} The above relations also allow expressing

342-443: A value of one volt , which is 1 J/C , multiplied by the elementary charge e  =  1.602 176 634 × 10  C . Therefore, one electronvolt is equal to 1.602 176 634 × 10  J . The electronvolt (eV) is a unit of energy, but is not an SI unit . It is a commonly used unit of energy within physics, widely used in solid state , atomic , nuclear and particle physics, and high-energy astrophysics . It

380-403: A wavelength of 532 nm (green light) would have an energy of approximately 2.33 eV . Similarly, 1 eV would correspond to an infrared photon of wavelength 1240 nm or frequency 241.8 THz . In a low-energy nuclear scattering experiment, it is conventional to refer to the nuclear recoil energy in units of eVr, keVr, etc. This distinguishes the nuclear recoil energy from

418-399: Is a Pythagorean equation . When a relatively high energy is applied to a particle with relatively low rest mass , it can be approximated as E ≃ p {\displaystyle E\simeq p} in high-energy physics such that an applied energy with expressed in the unit eV conveniently results in a numerically approximately equivalent change of momentum when expressed with

SECTION 10

#1732783267459

456-461: Is an SI unit. In the fields of physics in which the electronvolt is used, other quantities are typically measured using units derived from the electronvolt as a product with fundamental constants of importance in the theory are often used. By mass–energy equivalence , the electronvolt corresponds to a unit of mass . It is common in particle physics , where units of mass and energy are often interchanged, to express mass in units of eV/ c , where c

494-514: Is being converted in its atmosphere and magnetosphere. It is radiation-hardened to collect in situ data on the planet's auroral magnetic field lines, the equatorial magnetosphere, and the polar ionosphere. It was built by the Johns Hopkins University Applied Physics Laboratory (APL). One of the goals is to understand the aurorae, and how particles are accelerated to such high speeds. One of

532-436: Is commonly used with SI prefixes milli- (10 ), kilo- (10 ), mega- (10 ), giga- (10 ), tera- (10 ), peta- (10 ) or exa- (10 ), the respective symbols being meV, keV, MeV, GeV, TeV, PeV and EeV. The SI unit of energy is the joule (J). In some older documents, and in the name Bevatron , the symbol BeV is used, where the B stands for billion . The symbol BeV is therefore equivalent to GeV , though neither

570-794: Is convenient to use the electronvolt to express temperature. The electronvolt is divided by the Boltzmann constant to convert to the Kelvin scale : 1 e V / k B = 1.602   176   634 × 10 − 19  J 1.380   649 × 10 − 23  J/K = 11   604.518   12  K , {\displaystyle {1\,\mathrm {eV} /k_{\text{B}}}={1.602\ 176\ 634\times 10^{-19}{\text{ J}} \over 1.380\ 649\times 10^{-23}{\text{ J/K}}}=11\ 604.518\ 12{\text{ K}},} where k B

608-493: Is primarily concerned with the way in which electrons are arranged around the nucleus and the processes by which these arrangements change. This comprises ions , neutral atoms and, unless otherwise stated, it can be assumed that the term atom includes ions. The term atomic physics can be associated with nuclear power and nuclear weapons , due to the synonymous use of atomic and nuclear in standard English . Physicists distinguish between atomic physics—which deals with

646-441: Is the Boltzmann constant . The k B is assumed when using the electronvolt to express temperature, for example, a typical magnetic confinement fusion plasma is 15 keV (kiloelectronvolt), which is equal to 174 MK (megakelvin). As an approximation: k B T is about 0.025 eV (≈ ⁠ 290 K / 11604 K/eV ⁠ ) at a temperature of 20 °C . The energy E , frequency ν , and wavelength λ of

684-663: Is the Planck constant , c is the speed of light . This reduces to E = 4.135   667   696 × 10 − 15 e V / H z × ν = 1   239.841   98 e V ⋅ n m λ . {\displaystyle {\begin{aligned}E&=4.135\ 667\ 696\times 10^{-15}\;\mathrm {eV/Hz} \times \nu \\[4pt]&={\frac {1\ 239.841\ 98\;\mathrm {eV{\cdot }nm} }{\lambda }}.\end{aligned}}} A photon with

722-901: Is the speed of light in vacuum (from E = mc ). It is common to informally express mass in terms of eV as a unit of mass , effectively using a system of natural units with c set to 1. The kilogram equivalent of 1 eV/ c is: 1 eV / c 2 = ( 1.602   176   634 × 10 − 19 C ) × 1 V ( 299   792   458 m / s ) 2 = 1.782   661   92 × 10 − 36 kg . {\displaystyle 1\;{\text{eV}}/c^{2}={\frac {(1.602\ 176\ 634\times 10^{-19}\,{\text{C}})\times 1\,{\text{V}}}{(299\ 792\ 458\;\mathrm {m/s} )^{2}}}=1.782\ 661\ 92\times 10^{-36}\;{\text{kg}}.} For example, an electron and

760-447: Is the measure of an amount of kinetic energy gained by a single electron accelerating through an electric potential difference of one volt in vacuum . When used as a unit of energy , the numerical value of 1 eV in joules (symbol J) is equal to the numerical value of the charge of an electron in coulombs (symbol C). Under the 2019 revision of the SI , this sets 1 eV equal to

798-476: The Faraday constant ( F ≈ 96 485  C⋅mol ), where the energy in joules of n moles of particles each with energy E  eV is equal to E · F · n . Atomic physics Atomic physics is the field of physics that studies atoms as an isolated system of electrons and an atomic nucleus . Atomic physics typically refers to the study of atomic structure and the interaction between atoms. It

SECTION 20

#1732783267459

836-410: The mean lifetime τ of an unstable particle (in seconds) in terms of its decay width Γ (in eV) via Γ = ħ / τ . For example, the B meson has a lifetime of 1.530(9)  picoseconds , mean decay length is cτ = 459.7 μm , or a decay width of 4.302(25) × 10  eV . Conversely, the tiny meson mass differences responsible for meson oscillations are often expressed in

874-483: The periodic system of elements by Dmitri Mendeleev was another great step forward. The true beginning of atomic physics is marked by the discovery of spectral lines and attempts to describe the phenomenon, most notably by Joseph von Fraunhofer . The study of these lines led to the Bohr atom model and to the birth of quantum mechanics . In seeking to explain atomic spectra, an entirely new mathematical model of matter

912-483: The "electron equivalent" recoil energy (eVee, keVee, etc.) measured by scintillation light. For example, the yield of a phototube is measured in phe/keVee ( photoelectrons per keV electron-equivalent energy). The relationship between eV, eVr, and eVee depends on the medium the scattering takes place in, and must be established empirically for each material. One mole of particles given 1 eV of energy each has approximately 96.5 kJ of energy – this corresponds to

950-626: The Earth-orbiting Van Allen Probes (launched 2012), called RBSPICE, is nearly identical to JEDI. This type of instrument is also similar to the PEPSSI instrument on New Horizons (Pluto/Kupiter probe). JEDI, in combination with data from the Ultraviolet Spectrometer , detected electrical potentials of 400,000 electron volts (400 keV), 20–30 times higher than Earth, driving charged particles into

988-476: The atom as a system consisting of a nucleus and electrons—and nuclear physics , which studies nuclear reactions and special properties of atomic nuclei. As with many scientific fields, strict delineation can be highly contrived and atomic physics is often considered in the wider context of atomic, molecular, and optical physics . Physics research groups are usually so classified. Atomic physics primarily considers atoms in isolation. Atomic models will consist of

1026-876: The conversion to MKS system of units can be achieved by: p = 1 GeV / c = ( 1 × 10 9 ) × ( 1.602   176   634 × 10 − 19 C ) × ( 1 V ) 2.99   792   458 × 10 8 m / s = 5.344   286 × 10 − 19 kg ⋅ m / s . {\displaystyle p=1\;{\text{GeV}}/c={\frac {(1\times 10^{9})\times (1.602\ 176\ 634\times 10^{-19}\;{\text{C}})\times (1\;{\text{V}})}{2.99\ 792\ 458\times 10^{8}\;{\text{m}}/{\text{s}}}}=5.344\ 286\times 10^{-19}\;{\text{kg}}{\cdot }{\text{m}}/{\text{s}}.} In particle physics ,

1064-408: The electron in excess of this amount is converted to kinetic energy according to the conservation of energy . The atom is said to have undergone the process of ionization. If the electron absorbs a quantity of energy less than the binding energy, it will be transferred to an excited state. After a certain time, the electron in an excited state will "jump" (undergo a transition) to a lower state. In

1102-479: The exact value 1.602 176 634 × 10  J . Historically, the electronvolt was devised as a standard unit of measure through its usefulness in electrostatic particle accelerator sciences, because a particle with electric charge q gains an energy E = qV after passing through a voltage of V . An electronvolt is the amount of energy gained or lost by a single electron when it moves through an electric potential difference of one volt . Hence, it has

1140-404: The mass of a proton. To convert to electronvolt mass-equivalent, use the formula: By dividing a particle's kinetic energy in electronvolts by the fundamental constant c (the speed of light), one can describe the particle's momentum in units of eV/ c . In natural units in which the fundamental velocity constant c is numerically 1, the c may be informally be omitted to express momentum using

1178-985: The more convenient inverse picoseconds. Energy in electronvolts is sometimes expressed through the wavelength of light with photons of the same energy: 1 eV h c = 1.602   176   634 × 10 − 19 J ( 2.99   792   458 × 10 11 mm / s ) × ( 6.62   607   015 × 10 − 34 J ⋅ s ) ≈ 806.55439 mm − 1 . {\displaystyle {\frac {1\;{\text{eV}}}{hc}}={\frac {1.602\ 176\ 634\times 10^{-19}\;{\text{J}}}{(2.99\ 792\ 458\times 10^{11}\;{\text{mm}}/{\text{s}})\times (6.62\ 607\ 015\times 10^{-34}\;{\text{J}}{\cdot }{\text{s}})}}\thickapprox 806.55439\;{\text{mm}}^{-1}.} In certain fields, such as plasma physics , it

JEDI - Misplaced Pages Continue

1216-536: The mysteries of Jupiter is that X-rays are emitted from the poles, but do not seem to come from the auroral ring. Each detector has a field of view of 120 degrees by 12 degrees, and they are together positioned to provide a 360-degree (a full circle) view of the sky along that axis. The Juno spacecraft travels very rapidly in the close vicinity of Jupiter (up to 50 km/s) and also spins very slowly (2 RPM). JEDI can detected particles from 30 to 1000 keV including: In relation to other space missions, an instrument on

1254-440: The nucleus. These are normally in a ground state but can be excited by the absorption of energy from light ( photons ), magnetic fields , or interaction with a colliding particle (typically ions or other electrons). Electrons that populate a shell are said to be in a bound state . The energy necessary to remove an electron from its shell (taking it to infinity) is called the binding energy . Any quantity of energy absorbed by

1292-570: The polar regions of Jupiter. A scientific paper titled Juno observations of energetic charged particles over Jupiter's polar regions: Analysis of monodirectional and bidirectional electron beams included results from a close pass over Jupiter's poles in August 2016 for electrons (25–800 keV) and protons (10–1500 keV). The paper analyzed electron angular beams in the auroral regions. Electronvolt In physics , an electronvolt (symbol eV ), also written electron-volt and electron volt ,

1330-424: The released energy is transferred to another bound electron, causing it to go into the continuum. The Auger effect allows one to multiply ionize an atom with a single photon. There are rather strict selection rules as to the electronic configurations that can be reached by excitation by light — however, there are no such rules for excitation by collision processes. One of the earliest steps towards atomic physics

1368-441: The unit electronvolt. The energy–momentum relation E 2 = p 2 c 2 + m 0 2 c 4 {\displaystyle E^{2}=p^{2}c^{2}+m_{0}^{2}c^{4}} in natural units (with c = 1 {\displaystyle c=1} ) E 2 = p 2 + m 0 2 {\displaystyle E^{2}=p^{2}+m_{0}^{2}}

1406-404: The unit eV/ c . The dimension of momentum is T L M . The dimension of energy is T L M . Dividing a unit of energy (such as eV) by a fundamental constant (such as the speed of light) that has the dimension of velocity ( T L ) facilitates the required conversion for using a unit of energy to quantify momentum. For example, if the momentum p of an electron is 1 GeV/ c , then

1444-577: Was the recognition that matter was composed of atoms . It forms a part of the texts written in 6th century BC to 2nd century BC, such as those of Democritus or Vaiśeṣika Sūtra written by Kaṇāda . This theory was later developed in the modern sense of the basic unit of a chemical element by the British chemist and physicist John Dalton in the 18th century. At this stage, it wasn't clear what atoms were, although they could be described and classified by their properties (in bulk). The invention of

#458541