ភាពខុសគ្នារវាងកំណែនានារបស់ "ហែងរីហ ហឺត"

(r2.7.2) (រ៉ូបូ បន្ថែម: ky:Герц, Генрих Рудольф)
'''ហែងរីហ ហឺត''' ({{lang-en|Heinrich Rudolf Hertz}}) (២២ កុម្ភះកុម្ភៈ ១៨៥៧ – ១ មករា ១៨៩៤) ជា[[រូបវិទូ]]សញ្ជាតិ[[អាឡឺម៉ង់]]ដែលបានបកស្រាយ និងបន្លាយពង្រីកបន្លែមលើទ្រឺស្ដីនិងបន្លាយពង្រីកបន្ថែមលើទ្រឺស្ដី[[អេឡិចត្រូម៉ាញ៉េទិច]]នៃពន្លឺនៃ[[ពន្លឺ]] ដែលបានរកឃើញមុខដំបូងដោយ [[Jamesចេម Clerkឃ្លើក Maxwellម៉ាកស្វែល|Maxwellម៉ាកស្វែល]]។ គាត់ជាមនុស្សទីមួយដែលបានរកឃើញ[[រលកសញ្ញាវិទ្យុ]]ក្នុងឆ្នាំ១៨៨៨។ គាត់ក៏បានបកស្រាយនិងពន្យល់ថា ពន្លឺគឺជារលកសញ្ញាអេឡិចត្រូម៉ាញ៉េទិច។ ដូច្នេះហើយទើប ខ្នាតនៃ[[ប្រេកង់]] (ហឺត / Hz) យកតាមឈ្មោះរបស់គ្នា។
ហឺតចាប់កំណើតនៅរដ្ឋហាំបួក (Hamburg) ដែលជាអតីតរដ្ឋឯករាជមួយ​នៅក្នុង[[សហព័ន្ធអាល្លឺមង់]] ទៅក្នុងគ្រួសារមួយមានវណ្ណៈខ្ពស់ មានទ្រព្វសម្បត្តិស្ដុកស្ដម្ភ​និងកំរិតវប្បធម៌ខ្ពស់។ ឪពុករបស់គាត់ឈ្មោះ ហ្គាស្តាវ ហ្វែរឌីណាន់ ហឺត (Gustav Ferdinand Hertz) ជាអ្នកនិពន្ធសៀវភៅ​និងក្រោយមកក្លាយជាសមាជិកសភាជាតិ។ His mother was the former Anna Elisabeth Pfefferkorn. His paternal grandfather David Wolff Hertz (1757–1822), fourth son of Benjamin Wolff Hertz, moved to Hamburg in 1793 where he made his living as a jeweller. He and his wife Schöne Hertz (1760–1834) were buried in the former Jewish cemetery in Ottensen. Their first son Wolff Hertz (1790–1859), was chairman of the [[Jewish]] community. His brother Hertz Hertz (1797–1862) was a respected businessman. He was married to Betty Oppenheim, the daughter of the banker Salomon Oppenheim, from [[Cologne]]. Hertz converted from [[Judaism]] to [[Christianity]] and took the name Heinrich David Hertz.<ref>{{cite web|url=http://www1.uni-hamburg.de/rz3a035//bundesstrasse1.html |title=Buildings Integral to the Former Life and/or Persecution of Jews in Hamburg |publisher=.uni-hamburg.de |date= |accessdate=2012-02-22}}</ref>
While studying at the [[Gelehrtenschule des Johanneums]] in Hamburg, he showed an aptitude for sciences as well as languages, learning [[Arabic language|Arabic]] and [[Sanskrit]]. He studied sciences and engineering in the German cities of [[Dresden]], [[Technical University of Munich|Munich]] and [[Humboldt University of Berlin|Berlin]], where he studied under [[Gustav R. Kirchhoff]] and [[Hermann von Helmholtz]].
In 1880, Hertz obtained his [[PhD]] from the [[University of Berlin]]; and remained for post-doctoral study under [[Hermann von Helmholtz]].
In 1883, Hertz took a post as a lecturer in theoretical physics at the [[University of Kiel]].
In 1885, Hertz became a full professor at the [[University of Karlsruhe]] where he discovered electromagnetic waves.
The most dramatic prediction of [[James Clerk Maxwell|Maxwell]]'s theory of electromagnetism, published in 1865, was the existence of electromagnetic waves moving at the [[speed of light]], and the conclusion that light itself was just such a wave. This challenged experimentalists to generate and detect electromagnetic radiation using some form of electrical apparatus.
The first clearly successful attempt was made by Heinrich Hertz in 1886. For his radio wave transmitter he used a high [[voltage]] induction coil, a condenser (capacitor, Leyden jar) and a spark gap—whose poles on either side are formed by spheres of 2&nbsp;cm radius—to cause a spark discharge between the spark gap’s poles oscillating at a frequency determined by the values of the [[capacitor]] and the [[induction coil]].
To prove there really was [[radiation]] emitted, it had to be detected. Hertz used a piece of copper wire, 1&nbsp;mm thick, bent into a circle of a diameter of 7.5&nbsp;cm, with a small brass sphere on one end, and the other end of the wire was pointed, with the point near the sphere. He bought a screw mechanism so that the point could be moved very close to the sphere in a controlled fashion. This "receiver" was designed so that current oscillating back and forth in the wire would have a natural period close to that of the "transmitter" described above. The presence of [[oscillating]] charge in the receiver would be signaled by sparks across the (tiny) gap between the point and the sphere (typically, this gap was hundredths of a millimeter).
In more advanced experiments, Hertz measured the velocity of electromagnetic radiation and found it to be the same as the light’s velocity. He also showed that the nature of radio waves’ reflection and refraction was the same as those of light and established beyond any doubt that light is a form of electromagnetic radiation obeying the Maxwell equations.
Hertz's experiments would soon trigger the invention of the [[wireless telegraph]], [[radio]], and later [[television]]. In 1930 the [[International Electrotechnical Commission]] (IEC) recognized his work by naming the unit of frequency—one cycle per second—the "[[hertz]]".<ref name="hertzunit" />
He always had a deep interest in [[meteorology]] probably derived from his contacts with [[Wilhelm von Bezold]] (who was Hertz's professor in a laboratory course at the Munich Polytechnic in the summer of 1878). Hertz, however, did not contribute much to the field himself except some early articles as an assistant to Helmholtz in [[Berlin]], including research on the [[evaporation]] of [[liquid]]s, a new kind of [[hygrometer]], and a graphical means of determining the properties of moist air when subjected to [[adiabatic]] changes.<ref>Mulligan, J. F., and H. G. Hertz, "On the energy balance of the Earth," ''American Journal of Physics'', Vol. 65, pp. 36–45.</ref>
===Contact mechanics===
[[Image:Büste von Heinrich Hertz in Karlsruhe.jpg|thumb|Memorial of Heinrich Hertz on the campus of the [[Karlsruhe Institute of Technology]]]]
{{Main|Contact mechanics}}
In 1886–1889, Hertz published two articles on what was to become known as the field of [[contact mechanics]]. Hertz is well known for his contributions to the field of electrodynamics (''see below''); however, most papers that look into the fundamental nature of contact cite his two papers as a source for some important ideas. [[Joseph Valentin Boussinesq]] published some critically important observations on Hertz's work, nevertheless establishing this work on contact mechanics to be of immense importance. His work basically summarises how two [[axi-symmetric]] objects placed in contact will behave under [[loading]], he obtained results based upon the classical theory of [[elasticity]] and [[continuum mechanics]]. The most significant failure of his theory was the neglect of any nature of [[adhesion]] between the two solids, which proves to be important as the materials composing the solids start to assume high elasticity. It was natural to neglect adhesion in that age as there were no experimental methods of testing for it.
To develop his theory Hertz used his observation of elliptical [[Newton's rings]] formed upon placing a glass sphere upon a lens as the basis of assuming that the pressure exerted by the sphere follows an [[elliptical]] distribution. He used the formation of Newton's rings again while validating his theory with experiments in calculating the [[displacement]] which the sphere has into the lens. K. L. Johnson, K. Kendall and A. D. Roberts (JKR) used this theory as a basis while calculating the theoretical displacement or ''indentation depth'' in the presence of adhesion in their landmark article "Surface energy and contact of elastic solids" published in 1971 in the Proceedings of the Royal Society (A324, 1558, 301–313). Hertz's theory is recovered from their formulation if the adhesion of the materials is assumed to be zero. Similar to this theory, however using different assumptions, [[Boris Derjaguin|B. V. Derjaguin]], V. M. Muller and Y. P. Toporov published another theory in 1975, which came to be known as the DMT theory in the research community, which also recovered Hertz's formulations under the assumption of zero adhesion. This DMT theory proved to be rather premature and needed several revisions before it came to be accepted as another material contact theory in addition to the JKR theory. Both the DMT and the JKR theories form the basis of contact mechanics upon which all transition contact models are based and used in material parameter prediction in [[nanoindentation]] and [[atomic force microscopy]]. So Hertz's research from his days as a lecturer, preceding his great work on electromagnetism, which he himself considered with his characteristic soberness to be trivial, has come down to the age of [[nanotechnology]].
===Electromagnetic research===
[[File:Electric Waves being Research on the Propagation of Electric Action with Finite Velcity Through Space.jpg|left|thumb|Official English translation of ''Untersuchungen über die ausbreitung der elektrischen kraft'' published in 1893, a year before Hertz's death.]]
In 1886, Hertz developed the '''Hertz antenna''' receiver. This is a set of terminals which is not electrically grounded for its operation. He also developed a transmitting type of [[dipole antenna]], which was a center-fed driven element for transmitting [[ultra high frequency|UHF]] radio waves. These antennas are the simplest practical antennas from a theoretical point of view.
In 1887, Hertz experimented with radio waves in his laboratory. These actions followed [[Albert Abraham Michelson|Michelson's]] 1881 experiment (precursor to the 1887 [[Michelson–Morley experiment]]), which did not detect the existence of [[luminiferous aether|aether drift]]. Hertz altered [[Maxwell's equations]] to take this view into account for electromagnetism. Hertz used a [[Induction coil|Ruhmkorff coil]]-driven spark gap and one meter wire pair as a radiator. Capacity spheres were present at the ends for circuit resonance adjustments. His receiver, a precursor to the dipole antenna, was a simple half-wave [[dipole]] antenna for [[shortwave]]s. Hertz published his work in a book titled: ''Electric waves: being researches on the propagation of electric action with finite velocity through space''.<ref>[http://books.google.com/books?id=8GkOAAAAIAAJ&pg=PR3#v=onepage&q&f=false ''Electric waves: being researches on the propagation of electric action with finite velocity through space''], download here</ref>
[[Image:TransverseEMwave.PNG|center|Theoretical results from the 1887 experiment]]
Through experimentation, he proved that transverse [[free space]] [[electromagnetic wave]]s can travel over some distance. This had been predicted by [[James Clerk Maxwell]] and [[Michael Faraday]]. With his apparatus configuration, the electric and magnetic fields would radiate away from the wires as [[transverse waves]]. Hertz had positioned the [[oscillator]] about 12 meters from a [[zinc]] reflecting plate to produce [[standing wave]]s. Each wave was about 4 meters. Using the ring detector, he recorded how the [[amplitude|magnitude]] and wave's component direction vary. Hertz measured Maxwell's waves and demonstrated that the [[velocity]] of radio waves was equal to the velocity of light. The [[electric field intensity]] and [[Polarization (waves)|polarity]] was also measured by Hertz. (Hertz, 1887, 1888).
The [[Hertzian cone]] was first described by Hertz as a type of wave-front propagation through various [[Transmission medium|media]]. His experiments expanded the field of electromagnetic transmission and his apparatus was developed further by others in the radio. Hertz also found that [[radio waves]] could be transmitted through different types of materials, and were reflected by others, leading in the distant future to [[radar]].
Hertz helped establish the [[photoelectric]] effect (which was later explained by [[Albert Einstein]]) when he noticed that a [[electric charge|charged]] object loses its charge more readily when illuminated by ultraviolet light. In 1887, he made observations of the photoelectric effect and of the production and reception of electromagnetic (EM) waves, published in the journal [[Annalen der Physik]]. His receiver consisted of a coil with a [[spark gap]], whereby a spark would be seen upon detection of EM waves. He placed the apparatus in a darkened box to see the spark better. He observed that the maximum spark length was reduced when in the box. A glass panel placed between the source of EM waves and the receiver absorbed [[ultraviolet radiation]] that assisted the [[electron]]s in jumping across the gap.
[[Image:Hertz schematic0.PNG|right|333px|thumb|1887 experimental setup of Hertz's apparatus]]
When removed, the spark length would increase. He observed no decrease in spark length when he substituted quartz for glass, as [[quartz]] does not absorb UV radiation. Hertz concluded his months of investigation and reported the results obtained. He did not further pursue investigation of this effect, nor did he make any attempt at explaining how the observed phenomenon was brought about.
Hertz did not realize the practical importance of his experiments. He stated that,
: "''It's of no use whatsoever''[...]'' this is just an experiment that proves Maestro Maxwell was right—we just have these mysterious electromagnetic waves that we cannot see with the naked eye. But they are there.''"<ref name="huji">Institute of Chemistry, Hebrew University of Jerusalem: Hertz biography, digitized photographs. chem.ch.huji.ac.il/history/hertz.htm (Dead)</ref><ref>Anton Z. Capri, ''Quips, quotes, and quanta: an anecdotal history of physics''. 2007. Page 93.</ref><ref>Andrew Norton, ''Dynamic fields and waves''. 2000. Page 83.</ref>
Asked about the ramifications of his discoveries, Hertz replied,
: "''Nothing, I guess''."<ref name = "huji"/>
His discoveries would later be more fully understood by others and be part of the new "[[wireless|wireless age]]". In bulk, Hertz' experiments explain [[Reflection (electrical)|reflection]], [[refraction]], [[polarization]], [[Interference (wave propagation)|interference]], and velocity of [[electric wave]]s.
In 1892, Hertz began experimenting and demonstrated that [[cathode ray]]s could penetrate very thin metal foil (such as [[aluminium]]). [[Philipp Lenard]], a student of Heinrich Hertz, further researched this "[[X-rays|ray effect]]". He developed a version of the cathode tube and studied the penetration by X-rays of various materials. Philipp Lenard, though, did not realize that he was producing X-rays. Hermann von Helmholtz formulated mathematical equations for X-rays. He postulated a dispersion theory before [[Wilhelm Conrad Röntgen|Röntgen]] made his discovery and announcement. It was formed on the basis of the electromagnetic theory of light (''Wiedmann's Annalen'', Vol. XLVIII). However, he did not work with actual X-rays.
===Death at age 36===
In 1892, an infection was diagnosed (after a bout of severe migraines) and Hertz underwent some operations to correct the illness. He died of [[Wegener's granulomatosis]] at the age of 36 in [[Bonn]], Germany in 1894, and was buried in Ohlsdorf, Hamburg at the Jewish cemetery.<ref>For a photograph of his gravesite, see {{cite web | title = Heinrich Rudolf Hertz | url = http://phisicist.info/hertz.html | accessdate = 2008-12-02}} {{Dead link|date=September 2010|bot=H3llBot}}</ref>
Hertz's wife, Elizabeth Hertz (maiden name: Elizabeth Doll), did not remarry. Heinrich Hertz left two daughters, Joanna and Mathilde. Subsequently, all three women left Germany in the 1930s and went to England, after the rise of [[Adolf Hitler]]. Charles Susskind interviewed Mathilde Hertz in the 1960s and he later published a book on Heinrich Hertz. Heinrich Hertz's daughters never married and he does not have any descendants, according to the book by Susskind.
===Legacy and honors===
His nephew [[Gustav Ludwig Hertz]] was a [[Nobel Prize]] winner, and Gustav's son [[Carl Hellmuth Hertz]] invented [[medical ultrasonography]].
The SI unit ''[[hertz]]'' (Hz) was established in his honor by the IEC in 1930 for [[frequency]], an expression of the number of times that a repeated event occurs per second. It was adopted by the CGPM (Conférence générale des poids et mesures) in 1960, officially replacing the previous name, the "[[cycle per second]]" (cps).
In 1969 ([[East Germany]]), a Heinrich Hertz memorial medal<ref>http://highfields-arc.co.uk/biogs/hrhertz.htm</ref> was cast. The [[IEEE]] Heinrich Hertz Medal, established in 1987, is "''for outstanding achievements in Hertzian waves ''[...]'' presented annually to an individual for achievements which are theoretical or experimental in nature''".
[[File:Heinrich Hertz Deutsche-200-1Kcs.jpg|thumb|left|Heinrich Hertz]]
A [[Impact crater|crater]] that lies on the [[Far side (Moon)|far side]] of the [[Moon]], just behind the eastern limb, is [[Hertz (crater)|named in his honor]]. The Hertz market for radio electronics products in [[Nizhny Novgorod]], Russia, is named after him. The [[Heinrich-Hertz-Turm]] radio telecommunication tower in Hamburg is named after the city's famous son.
Hertz is honored by Japan with a membership in the [[Order of the Sacred Treasure]], which has multiple layers of honor for prominent people, including scientists.<ref>L'Harmattan: [http://www.editions-harmattan.fr/index.asp?navig=catalogue&obj=article&no=8245 List of recipients of Japanese Order of the Sacred Treasure (in French)]</ref>
Heinrich Hertz has been honored by a number of countries around the world in their postage issues, and in post-World War II times has appeared on various German stamp issues as well.
On his birthday in 2012, [[Google]] honored Hertz with a [[Google doodle]] inspired by his life's work on its home page.<ref>{{Citation |last= Albanesius |first= Chloe |publication-date= February 22, 2012 |title= Google Doodle Honors Heinrich Hertz, Electromagnetic Wave Pioneer |work= pcmag.com |url= http://www.pcmag.com/article2/0,2817,2400529,00.asp |accessdate= February 22, 2012 }}</ref>
===Nazi revisionism===
Although Hertz would not have considered himself [[Jewish]], his "Jewish" portrait was removed by the [[Nazi]]s from its prominent position of honor in [[Hamburg Rathaus|Hamburg's City Hall (''Rathaus'')]] because of his partly "Jewish ancestry." Hertz was a Lutheran; and although his father’s family had been Jewish,<ref name="DSB340">Koertge, Noretta. (2007). ''Dictionary of Scientific Biography,'' Vol. 6, p. 340.</ref> his father had converted to Catholicism before marrying.{{Citation needed|date=January 2011}} The painting has since been returned to public display.<ref>Robertson, Struan: [http://www1.uni-hamburg.de/rz3a035//hertz.html Hertz biography]</ref>