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74-420: PNE can be used to abbreviate the subatomic particles, Proton , Neutron and Electron , when referring to them en masse . PNE as an acronym could refer to: Proton One or more protons are present in the nucleus of every atom . They provide the attractive electrostatic central force which binds the atomic electrons. The number of protons in the nucleus is the defining property of an element, and

148-400: A {\displaystyle a} , and τ p {\displaystyle \tau _{\mathrm {p} }} decreases with increasing a {\displaystyle a} . Acceleration gives rise to a non-vanishing probability for the transition p → n + e + ν e . This was a matter of concern in

222-487: A proton is composed of two up quarks (each with electric charge + + 2 ⁄ 3 , for a total of + 4 ⁄ 3 together) and one down quark (with electric charge − + 1 ⁄ 3 ). Adding these together yields the proton charge of +1. Although quarks also carry color charge , hadrons must have zero total color charge because of a phenomenon called color confinement . That is, hadrons must be "colorless" or "white". The simplest ways for this to occur are with

296-427: A zinc sulfide screen produced at a distance well beyond the distance of alpha-particle range of travel but instead corresponding to the range of travel of hydrogen atoms (protons). After experimentation, Rutherford traced the reaction to the nitrogen in air and found that when alpha particles were introduced into pure nitrogen gas, the effect was larger. In 1919, Rutherford assumed that the alpha particle merely knocked

370-449: A bare nucleus, consisting of a proton (and 0 neutrons for the most abundant isotope protium 1 H ). The proton is a "bare charge" with only about 1/64,000 of the radius of a hydrogen atom, and so is extremely reactive chemically. The free proton, thus, has an extremely short lifetime in chemical systems such as liquids and it reacts immediately with the electron cloud of any available molecule. In aqueous solution, it forms

444-416: A form-factor related to the two-dimensional parton diameter of the proton. A value from before 2010 is based on scattering electrons from protons followed by complex calculation involving scattering cross section based on Rosenbluth equation for momentum-transfer cross section ), and based on studies of the atomic energy levels of hydrogen and deuterium. In 2010 an international research team published

518-484: A neutral hydrogen atom , which is chemically a free radical . Such "free hydrogen atoms" tend to react chemically with many other types of atoms at sufficiently low energies. When free hydrogen atoms react with each other, they form neutral hydrogen molecules (H 2 ), which are the most common molecular component of molecular clouds in interstellar space . Free protons are routinely used for accelerators for proton therapy or various particle physics experiments, with

592-527: A new category term: Notwithstanding the fact that this report deals with weak interactions, we shall frequently have to speak of strongly interacting particles. These particles pose not only numerous scientific problems, but also a terminological problem. The point is that " strongly interacting particles " is a very clumsy term which does not yield itself to the formation of an adjective. For this reason, to take but one instance, decays into strongly interacting particles are called "non- leptonic ". This definition

666-543: A number of situations in which energies or temperatures are high enough to separate them from electrons, for which they have some affinity. Free protons exist in plasmas in which temperatures are too high to allow them to combine with electrons . Free protons of high energy and velocity make up 90% of cosmic rays , which propagate through the interstellar medium . Free protons are emitted directly from atomic nuclei in some rare types of radioactive decay . Protons also result (along with electrons and antineutrinos ) from

740-461: A proton charge radius measurement via the Lamb shift in muonic hydrogen (an exotic atom made of a proton and a negatively charged muon ). As a muon is 200 times heavier than an electron, resulting in a smaller atomic orbital , it is much more sensitive to the proton's charge radius and thus allows a more precise measurement. Subsequent improved scattering and electron-spectroscopy measurements agree with

814-418: A proton out of nitrogen, turning it into carbon. After observing Blackett's cloud chamber images in 1925, Rutherford realized that the alpha particle was absorbed. If the alpha particle were not absorbed, then it would knock a proton off of nitrogen creating 3 charged particles (a negatively charged carbon, a proton, and an alpha particle). It can be shown that the 3 charged particles would create three tracks in

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888-697: A proton's mass. The remainder of a proton's mass is due to quantum chromodynamics binding energy , which includes the kinetic energy of the quarks and the energy of the gluon fields that bind the quarks together. The root mean square charge radius of a proton is about 0.84–0.87  fm ( 1 fm = 10  m ). In 2019, two different studies, using different techniques, found this radius to be 0.833 fm, with an uncertainty of ±0.010 fm. Free protons occur occasionally on Earth: thunderstorms can produce protons with energies of up to several tens of MeV . At sufficiently low temperatures and kinetic energies, free protons will bind to electrons . However,

962-425: A quark of one color and an antiquark of the corresponding anticolor, or three quarks of different colors. Hadrons with the first arrangement are a type of meson , and those with the second arrangement are a type of baryon . Massless virtual gluons compose the overwhelming majority of particles inside hadrons, as well as the major constituents of its mass (with the exception of the heavy charm and bottom quarks ;

1036-547: A result, they become so-called Brønsted acids . For example, a proton captured by a water molecule in water becomes hydronium , the aqueous cation H 3 O . In chemistry , the number of protons in the nucleus of an atom is known as the atomic number , which determines the chemical element to which the atom belongs. For example, the atomic number of chlorine is 17; this means that each chlorine atom has 17 protons and that all atoms with 17 protons are chlorine atoms. The chemical properties of each atom are determined by

1110-455: A simplistic interpretation of early values of atomic weights (see Prout's hypothesis ), which was disproved when more accurate values were measured. In 1886, Eugen Goldstein discovered canal rays (also known as anode rays) and showed that they were positively charged particles (ions) produced from gases. However, since particles from different gases had different values of charge-to-mass ratio ( q / m ), they could not be identified with

1184-431: A single particle, unlike the negative electrons discovered by J. J. Thomson . Wilhelm Wien in 1898 identified the hydrogen ion as the particle with the highest charge-to-mass ratio in ionized gases. Following the discovery of the atomic nucleus by Ernest Rutherford in 1911, Antonius van den Broek proposed that the place of each element in the periodic table (its atomic number) is equal to its nuclear charge. This

1258-487: Is a lone proton. The nuclei of the heavy hydrogen isotopes deuterium and tritium contain one proton bound to one and two neutrons, respectively. All other types of atomic nuclei are composed of two or more protons and various numbers of neutrons. The concept of a hydrogen-like particle as a constituent of other atoms was developed over a long period. As early as 1815, William Prout proposed that all atoms are composed of hydrogen atoms (which he called "protyles"), based on

1332-441: Is a unique chemical species, being a bare nucleus. As a consequence it has no independent existence in the condensed state and is invariably found bound by a pair of electrons to another atom. Ross Stewart, The Proton: Application to Organic Chemistry (1985, p. 1) In chemistry, the term proton refers to the hydrogen ion, H . Since the atomic number of hydrogen is 1, a hydrogen ion has no electrons and corresponds to

1406-426: Is found to be equal and opposite to that of a proton. Hadron In particle physics , a hadron ( / ˈ h æ d r ɒ n / ; from Ancient Greek ἁδρός (hadrós)  'stout, thick') is a composite subatomic particle made of two or more quarks held together by the strong interaction . They are analogous to molecules , which are held together by the electric force . Most of

1480-835: Is known as asymptotic freedom , has been experimentally confirmed in the energy range between 1  GeV (gigaelectronvolt) and 1  TeV (teraelectronvolt). All free hadrons except ( possibly ) the proton and antiproton are unstable . Baryons are hadrons containing an odd number of valence quarks (at least 3). Most well-known baryons such as the proton and neutron have three valence quarks, but pentaquarks with five quarks—three quarks of different colors, and also one extra quark-antiquark pair—have also been proven to exist. Because baryons have an odd number of quarks, they are also all fermions , i.e. , they have half-integer spin . As quarks possess baryon number B  =  1 ⁄ 3 , baryons have baryon number B  = 1. Pentaquarks also have B  = 1, since

1554-547: Is not exact because "non-leptonic" may also signify photonic. In this report I shall call strongly interacting particles "hadrons", and the corresponding decays "hadronic" (the Greek ἁδρός signifies "large", "massive", in contrast to λεπτός which means "small", "light"). I hope that this terminology will prove to be convenient. — L. B. Okun (1962) According to the quark model , the properties of hadrons are primarily determined by their so-called valence quarks . For example,

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1628-402: Is not meaningful to ask which quark is real and which virtual; only the small excess is apparent from the outside in the form of a hadron. Therefore, when a hadron or anti-hadron is stated to consist of (typically) two or three quarks, this technically refers to the constant excess of quarks versus antiquarks. Like all subatomic particles , hadrons are assigned quantum numbers corresponding to

1702-469: Is referred to as the atomic number (represented by the symbol Z ). Since each element is identified by the number of protons in its nucleus, each element has its own atomic number, which determines the number of atomic electrons and consequently the chemical characteristics of the element. The word proton is Greek for "first", and the name was given to the hydrogen nucleus by Ernest Rutherford in 1920. In previous years, Rutherford had discovered that

1776-512: Is reversible; neutrons can convert back to protons through beta decay , a common form of radioactive decay . In fact, a free neutron decays this way, with a mean lifetime of about 15 minutes. A proton can also transform into a neutron through beta plus decay (β+ decay). According to quantum field theory , the mean proper lifetime of protons τ p {\displaystyle \tau _{\mathrm {p} }} becomes finite when they are accelerating with proper acceleration

1850-515: The LHCb collaboration. Mesons are hadrons containing an even number of valence quarks (at least two). Most well known mesons are composed of a quark-antiquark pair, but possible tetraquarks (four quarks) and hexaquarks (six quarks, comprising either a dibaryon or three quark-antiquark pairs) may have been discovered and are being investigated to confirm their nature. Several other hypothetical types of exotic meson may exist which do not fall within

1924-519: The LHCb collaboration. There are several more exotic hadron candidates and other colour-singlet quark combinations that may also exist. Almost all "free" hadrons and antihadrons (meaning, in isolation and not bound within an atomic nucleus ) are believed to be unstable and eventually decay into other particles. The only known possible exception is free protons, which appear to be stable , or at least, take immense amounts of time to decay (order of 10  years). By way of comparison, free neutrons are

1998-583: The Morris water maze . Electrical charging of a spacecraft due to interplanetary proton bombardment has also been proposed for study. There are many more studies that pertain to space travel, including galactic cosmic rays and their possible health effects , and solar proton event exposure. The American Biostack and Soviet Biorack space travel experiments have demonstrated the severity of molecular damage induced by heavy ions on microorganisms including Artemia cysts. CPT-symmetry puts strong constraints on

2072-591: The constituent quark model, which were popular in the 1980s, and the SVZ sum rules , which allow for rough approximate mass calculations. These methods do not have the same accuracy as the more brute-force lattice QCD methods, at least not yet. The CODATA recommended value of a proton's charge radius is 8.4075(64) × 10  m . The radius of the proton is defined by a formula that can be calculated by quantum electrodynamics and be derived from either atomic spectroscopy or by electron–proton scattering. The formula involves

2146-462: The electron cloud in a normal atom. However, in such an association with an electron, the character of the bound proton is not changed, and it remains a proton. The attraction of low-energy free protons to any electrons present in normal matter (such as the electrons in normal atoms) causes free protons to stop and to form a new chemical bond with an atom. Such a bond happens at any sufficiently "cold" temperature (that is, comparable to temperatures at

2220-766: The hydrogen nucleus (known to be the lightest nucleus) could be extracted from the nuclei of nitrogen by atomic collisions. Protons were therefore a candidate to be a fundamental or elementary particle , and hence a building block of nitrogen and all other heavier atomic nuclei. Although protons were originally considered to be elementary particles, in the modern Standard Model of particle physics , protons are known to be composite particles, containing three valence quarks , and together with neutrons are now classified as hadrons . Protons are composed of two up quarks of charge + ⁠ 2 / 3 ⁠ e each, and one down quark of charge − ⁠ 1 / 3 ⁠ e . The rest masses of quarks contribute only about 1% of

2294-414: The hydronium ion , H 3 O , which in turn is further solvated by water molecules in clusters such as [H 5 O 2 ] and [H 9 O 4 ] . The transfer of H in an acid–base reaction is usually referred to as "proton transfer". The acid is referred to as a proton donor and the base as a proton acceptor. Likewise, biochemical terms such as proton pump and proton channel refer to

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2368-415: The longest-lived unstable particle , and decay with a half-life of about 611 seconds, and have a mean lifetime of 879 seconds, see free neutron decay . Hadron physics is studied by colliding hadrons, e.g. protons, with each other or the nuclei of dense, heavy elements , such as lead (Pb) or gold (Au), and detecting the debris in the produced particle showers . A similar process occurs in

2442-470: The mass of ordinary matter comes from two hadrons: the proton and the neutron , while most of the mass of the protons and neutrons is in turn due to the binding energy of their constituent quarks, due to the strong force. Hadrons are categorized into two broad families: baryons , made of an odd number of quarks (usually three) and mesons , made of an even number of quarks (usually two: one quark and one antiquark ). Protons and neutrons (which make

2516-686: The mean lifetime of a proton for various assumed decay products. Experiments at the Super-Kamiokande detector in Japan gave lower limits for proton mean lifetime of 6.6 × 10  years for decay to an antimuon and a neutral pion , and 8.2 × 10  years for decay to a positron and a neutral pion. Another experiment at the Sudbury Neutrino Observatory in Canada searched for gamma rays resulting from residual nuclei resulting from

2590-480: The radioactive decay of free neutrons , which are unstable. The spontaneous decay of free protons has never been observed, and protons are therefore considered stable particles according to the Standard Model. However, some grand unified theories (GUTs) of particle physics predict that proton decay should take place with lifetimes between 10 and 10 years. Experimental searches have established lower bounds on

2664-472: The representations of the Poincaré group : J ( m ), where J is the spin quantum number, P the intrinsic parity (or P-parity ), C the charge conjugation (or C-parity ), and m is the particle's mass . Note that the mass of a hadron has very little to do with the mass of its valence quarks; rather, due to mass–energy equivalence , most of the mass comes from the large amount of energy associated with

2738-718: The strong interaction . Hadrons may also carry flavor quantum numbers such as isospin ( G-parity ), and strangeness . All quarks carry an additive, conserved quantum number called a baryon number ( B ), which is + + 1 ⁄ 3 for quarks and − + 1 ⁄ 3 for antiquarks. This means that baryons (composite particles made of three, five or a larger odd number of quarks) have B  = 1 whereas mesons have B  = 0. Hadrons have excited states known as resonances . Each ground state hadron may have several excited states; several hundred different resonances have been observed in experiments. Resonances decay extremely quickly (within about 10   seconds ) via

2812-484: The top quark vanishes before it has time to bind into a hadron). The strength of the strong-force gluons which bind the quarks together has sufficient energy ( E ) to have resonances composed of massive ( m ) quarks ( E ≥ mc ). One outcome is that short-lived pairs of virtual quarks and antiquarks are continually forming and vanishing again inside a hadron. Because the virtual quarks are not stable wave packets (quanta), but an irregular and transient phenomenon, it

2886-518: The Moon is inside the Earth's geomagnetic tail, and typically no solar wind particles were detectable. For the remainder of each lunar orbit, the Moon is in a transitional region known as the magnetosheath , where the Earth's magnetic field affects the solar wind, but does not completely exclude it. In this region, the particle flux is reduced, with typical proton velocities of 250 to 450 kilometers per second. During

2960-407: The character of such bound protons does not change, and they remain protons. A fast proton moving through matter will slow by interactions with electrons and nuclei, until it is captured by the electron cloud of an atom. The result is a diatomic or polyatomic ion containing hydrogen. In a vacuum, when free electrons are present, a sufficiently slow proton may pick up a single free electron, becoming

3034-399: The cloud chamber, but instead only 2 tracks in the cloud chamber were observed. The alpha particle is absorbed by the nitrogen atom. After capture of the alpha particle, a hydrogen nucleus is ejected, creating a net result of 2 charged particles (a proton and a positively charged oxygen) which make 2 tracks in the cloud chamber. Heavy oxygen ( O), not carbon or fluorine, is the product. This was

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3108-480: The coaccelerated frame there is a thermal bath due to Fulling–Davies–Unruh effect , an intrinsic effect of quantum field theory. In this thermal bath, experienced by the proton, there are electrons and antineutrinos with which the proton may interact according to the processes: Adding the contributions of each of these processes, one should obtain τ p {\displaystyle \tau _{\mathrm {p} }} . In quantum chromodynamics ,

3182-438: The decay of a proton from oxygen-16. This experiment was designed to detect decay to any product, and established a lower limit to a proton lifetime of 2.1 × 10  years . However, protons are known to transform into neutrons through the process of electron capture (also called inverse beta decay ). For free protons, this process does not occur spontaneously but only when energy is supplied. The equation is: The process

3256-488: The extra quark's and antiquark's baryon numbers cancel. Each type of baryon has a corresponding antiparticle (antibaryon) in which quarks are replaced by their corresponding antiquarks. For example, just as a proton is made of two up quarks and one down quark, its corresponding antiparticle, the antiproton, is made of two up antiquarks and one down antiquark. As of August 2015, there are two known pentaquarks, P c (4380) and P c (4450) , both discovered in 2015 by

3330-441: The first reported nuclear reaction , N + α → O + p . Rutherford at first thought of our modern "p" in this equation as a hydrogen ion, H . Depending on one's perspective, either 1919 (when it was seen experimentally as derived from another source than hydrogen) or 1920 (when it was recognized and proposed as an elementary particle) may be regarded as the moment when the proton was 'discovered'. Rutherford knew hydrogen to be

3404-418: The gluons, and transitory pairs of sea quarks . Protons have a positive charge distribution, which decays approximately exponentially, with a root mean square charge radius of about 0.8 fm. Protons and neutrons are both nucleons , which may be bound together by the nuclear force to form atomic nuclei . The nucleus of the most common isotope of the hydrogen atom (with the chemical symbol "H")

3478-429: The later 1990s because τ p {\displaystyle \tau _{\mathrm {p} }} is a scalar that can be measured by the inertial and coaccelerated observers . In the inertial frame , the accelerating proton should decay according to the formula above. However, according to the coaccelerated observer the proton is at rest and hence should not decay. This puzzle is solved by realizing that in

3552-447: The lunar night, the spectrometer was shielded from the solar wind by the Moon and no solar wind particles were measured. Protons also have extrasolar origin from galactic cosmic rays , where they make up about 90% of the total particle flux. These protons often have higher energy than solar wind protons, and their intensity is far more uniform and less variable than protons coming from the Sun,

3626-612: The majority of the mass of an atom ) are examples of baryons; pions are an example of a meson. "Exotic" hadrons , containing more than three valence quarks, have been discovered in recent years. A tetraquark state (an exotic meson ), named the Z(4430) , was discovered in 2007 by the Belle Collaboration and confirmed as a resonance in 2014 by the LHCb collaboration. Two pentaquark states ( exotic baryons ), named P c (4380) and P c (4450) , were discovered in 2015 by

3700-402: The mass of a quark by itself, while constituent quark mass refers to the current quark mass plus the mass of the gluon particle field surrounding the quark. These masses typically have very different values. The kinetic energy of the quarks that is a consequence of confinement is a contribution (see Mass in special relativity ). Using lattice QCD calculations, the contributions to

3774-2129: The mass of the proton are the quark condensate (~9%, comprising the up and down quarks and a sea of virtual strange quarks), the quark kinetic energy (~32%), the gluon kinetic energy (~37%), and the anomalous gluonic contribution (~23%, comprising contributions from condensates of all quark flavors). The constituent quark model wavefunction for the proton is | p ↑ ⟩ = 1 18 ( 2 | u ↑ d ↓ u ↑ ⟩ + 2 | u ↑ u ↑ d ↓ ⟩ + 2 | d ↓ u ↑ u ↑ ⟩ − | u ↑ u ↓ d ↑ ⟩ − | u ↑ d ↑ u ↓ ⟩ − | u ↓ d ↑ u ↑ ⟩ − | d ↑ u ↓ u ↑ ⟩ − | d ↑ u ↑ u ↓ ⟩ − | u ↓ u ↑ d ↑ ⟩ ) . {\displaystyle \mathrm {|p_{\uparrow }\rangle ={\tfrac {1}{\sqrt {18}}}\left(2|u_{\uparrow }d_{\downarrow }u_{\uparrow }\rangle +2|u_{\uparrow }u_{\uparrow }d_{\downarrow }\rangle +2|d_{\downarrow }u_{\uparrow }u_{\uparrow }\rangle -|u_{\uparrow }u_{\downarrow }d_{\uparrow }\rangle -|u_{\uparrow }d_{\uparrow }u_{\downarrow }\rangle -|u_{\downarrow }d_{\uparrow }u_{\uparrow }\rangle -|d_{\uparrow }u_{\downarrow }u_{\uparrow }\rangle -|d_{\uparrow }u_{\uparrow }u_{\downarrow }\rangle -|u_{\downarrow }u_{\uparrow }d_{\uparrow }\rangle \right)} .} The internal dynamics of protons are complicated, because they are determined by

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3848-477: The modern theory of the nuclear force, most of the mass of protons and neutrons is explained by special relativity . The mass of a proton is about 80–100 times greater than the sum of the rest masses of its three valence quarks , while the gluons have zero rest mass. The extra energy of the quarks and gluons in a proton, as compared to the rest energy of the quarks alone in the QCD vacuum , accounts for almost 99% of

3922-475: The most powerful example being the Large Hadron Collider . Protons are spin- ⁠ 1 / 2 ⁠ fermions and are composed of three valence quarks, making them baryons (a sub-type of hadrons ). The two up quarks and one down quark of a proton are held together by the strong force , mediated by gluons . A modern perspective has a proton composed of the valence quarks (up, up, down),

3996-440: The movement of hydrated H ions. The ion produced by removing the electron from a deuterium atom is known as a deuteron , not a proton. Likewise, removing an electron from a tritium atom produces a triton . Also in chemistry, the term proton NMR refers to the observation of hydrogen-1 nuclei in (mostly organic ) molecules by nuclear magnetic resonance . This method uses the quantized spin magnetic moment of

4070-401: The natural environment, in the extreme upper-atmosphere, where muons and mesons such as pions are produced by the collisions of cosmic rays with rarefied gas particles in the outer atmosphere. The term "hadron" is a new Greek word introduced by L. B. Okun in a plenary talk at the 1962 International Conference on High Energy Physics at CERN . He opened his talk with the definition of

4144-438: The neutral hydrogen atom. He initially suggested both proton and prouton (after Prout). Rutherford later reported that the meeting had accepted his suggestion that the hydrogen nucleus be named the "proton", following Prout's word "protyle". The first use of the word "proton" in the scientific literature appeared in 1920. One or more bound protons are present in the nucleus of every atom. Free protons are found naturally in

4218-403: The new small radius. Work continues to refine and check this new value. Since the proton is composed of quarks confined by gluons, an equivalent pressure that acts on the quarks can be defined. The size of that pressure and other details about it are controversial. In 2018 this pressure was reported to be on the order 10  Pa, which is greater than the pressure inside a neutron star . It

4292-416: The nucleon structure is still missing because ... long-distance behavior requires a nonperturbative and/or numerical treatment ..." More conceptual approaches to the structure of protons are: the topological soliton approach originally due to Tony Skyrme and the more accurate AdS/QCD approach that extends it to include a string theory of gluons, various QCD-inspired models like the bag model and

4366-531: The nucleus the proton , after the neuter singular of the Greek word for "first", πρῶτον . However, Rutherford also had in mind the word protyle as used by Prout. Rutherford spoke at the British Association for the Advancement of Science at its Cardiff meeting beginning 24 August 1920. At the meeting, he was asked by Oliver Lodge for a new name for the positive hydrogen nucleus to avoid confusion with

4440-681: The number of (negatively charged) electrons , which for neutral atoms is equal to the number of (positive) protons so that the total charge is zero. For example, a neutral chlorine atom has 17 protons and 17 electrons, whereas a Cl anion has 17 protons and 18 electrons for a total charge of −1. All atoms of a given element are not necessarily identical, however. The number of neutrons may vary to form different isotopes , and energy levels may differ, resulting in different nuclear isomers . For example, there are two stable isotopes of chlorine : 17 Cl with 35 − 17 = 18 neutrons and 17 Cl with 37 − 17 = 20 neutrons. The proton

4514-701: The particles in the solar wind are electrons and protons, in approximately equal numbers. Because the Solar Wind Spectrometer made continuous measurements, it was possible to measure how the Earth's magnetic field affects arriving solar wind particles. For about two-thirds of each orbit, the Moon is outside of the Earth's magnetic field. At these times, a typical proton density was 10 to 20 per cubic centimeter, with most protons having velocities between 400 and 650 kilometers per second. For about five days of each month,

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4588-671: The pressure profile shape by selection of the model. The radius of the hydrated proton appears in the Born equation for calculating the hydration enthalpy of hydronium . Although protons have affinity for oppositely charged electrons, this is a relatively low-energy interaction and so free protons must lose sufficient velocity (and kinetic energy ) in order to become closely associated and bound to electrons. High energy protons, in traversing ordinary matter, lose energy by collisions with atomic nuclei , and by ionization of atoms (removing electrons) until they are slowed sufficiently to be captured by

4662-662: The production of which is heavily affected by solar proton events such as coronal mass ejections . Research has been performed on the dose-rate effects of protons, as typically found in space travel , on human health. To be more specific, there are hopes to identify what specific chromosomes are damaged, and to define the damage, during cancer development from proton exposure. Another study looks into determining "the effects of exposure to proton irradiation on neurochemical and behavioral endpoints, including dopaminergic functioning, amphetamine -induced conditioned taste aversion learning, and spatial learning and memory as measured by

4736-400: The proton's mass. The rest mass of a proton is, thus, the invariant mass of the system of moving quarks and gluons that make up the particle, and, in such systems, even the energy of massless particles confined to a system is still measured as part of the rest mass of the system. Two terms are used in referring to the mass of the quarks that make up protons: current quark mass refers to

4810-479: The proton, which is due to its angular momentum (or spin ), which in turn has a magnitude of one-half the reduced Planck constant . ( ℏ / 2 {\displaystyle \hbar /2} ). The name refers to examination of protons as they occur in protium (hydrogen-1 atoms) in compounds, and does not imply that free protons exist in the compound being studied. The Apollo Lunar Surface Experiments Packages (ALSEP) determined that more than 95% of

4884-447: The quark model of classification. These include glueballs and hybrid mesons (mesons bound by excited gluons ). Because mesons have an even number of quarks, they are also all bosons , with integer spin , i.e. , 0, +1, or −1. They have baryon number B = ⁠ 1 / 3 ⁠ − ⁠ 1 / 3 ⁠ = 0 . Examples of mesons commonly produced in particle physics experiments include pions and kaons . Pions also play

4958-513: The quarks' exchanging gluons, and interacting with various vacuum condensates. Lattice QCD provides a way of calculating the mass of a proton directly from the theory to any accuracy, in principle. The most recent calculations claim that the mass is determined to better than 4% accuracy, even to 1% accuracy (see Figure S5 in Dürr et al. ). These claims are still controversial, because the calculations cannot yet be done with quarks as light as they are in

5032-444: The real world. This means that the predictions are found by a process of extrapolation , which can introduce systematic errors. It is hard to tell whether these errors are controlled properly, because the quantities that are compared to experiment are the masses of the hadrons , which are known in advance. These recent calculations are performed by massive supercomputers, and, as noted by Boffi and Pasquini: "a detailed description of

5106-581: The relative properties of particles and antiparticles and, therefore, is open to stringent tests. For example, the charges of a proton and antiproton must sum to exactly zero. This equality has been tested to one part in 10 . The equality of their masses has also been tested to better than one part in 10 . By holding antiprotons in a Penning trap , the equality of the charge-to-mass ratio of protons and antiprotons has been tested to one part in 6 × 10 . The magnetic moment of antiprotons has been measured with an error of 8 × 10 nuclear Bohr magnetons , and

5180-443: The simplest and lightest element and was influenced by Prout's hypothesis that hydrogen was the building block of all elements. Discovery that the hydrogen nucleus is present in other nuclei as an elementary particle led Rutherford to give the hydrogen nucleus H a special name as a particle, since he suspected that hydrogen, the lightest element, contained only one of these particles. He named this new fundamental building block of

5254-416: The strong nuclear force. In other phases of matter the hadrons may disappear. For example, at very high temperature and high pressure, unless there are sufficiently many flavors of quarks, the theory of quantum chromodynamics (QCD) predicts that quarks and gluons will no longer be confined within hadrons, "because the strength of the strong interaction diminishes with energy ". This property, which

5328-482: The surface of the Sun) and with any type of atom. Thus, in interaction with any type of normal (non-plasma) matter, low-velocity free protons do not remain free but are attracted to electrons in any atom or molecule with which they come into contact, causing the proton and molecule to combine. Such molecules are then said to be " protonated ", and chemically they are simply compounds of hydrogen, often positively charged. Often, as

5402-525: Was confirmed experimentally by Henry Moseley in 1913 using X-ray spectra (More details in Atomic number under Moseley's 1913 experiment). In 1917, Rutherford performed experiments (reported in 1919 and 1925) which proved that the hydrogen nucleus is present in other nuclei, a result usually described as the discovery of protons. These experiments began after Rutherford observed that when alpha particles would strike air, Rutherford could detect scintillation on

5476-436: Was said to be maximum at the centre, positive (repulsive) to a radial distance of about 0.6 fm, negative (attractive) at greater distances, and very weak beyond about 2 fm. These numbers were derived by a combination of a theoretical model and experimental Compton scattering of high-energy electrons. However, these results have been challenged as also being consistent with zero pressure and as effectively providing

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