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Rifles, Reloading, Optics, Equipment
Long Range Scopes and Other Optics
Swaro vs Huskemaw
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<blockquote data-quote="RichCoyle" data-source="post: 2886511" data-attributes="member: 127134"><p>Maybe you could translate that into hunter talk.</p><p></p><p>[h1]Rayleigh law[/h1]<p>1 language</p><p></p><p></p><p>From Wikipedia, the free encyclopedia</p><p></p><p><em>This article is about the magnetic law. For the stochastic distribution, see <a href="https://en.wikipedia.org/wiki/Rayleigh_distribution" target="_blank">Rayleigh distribution</a>. For optical scattering, see <a href="https://en.wikipedia.org/wiki/Rayleigh_scattering" target="_blank">Rayleigh scattering</a>. For wireless multipath propagation, see <a href="https://en.wikipedia.org/wiki/Rayleigh_fading" target="_blank">Rayleigh fading</a>.</em></p><p>The <strong>Rayleigh law</strong> describes the behavior of <a href="https://en.wikipedia.org/wiki/Ferromagnetic" target="_blank">ferromagnetic</a> materials at low <a href="https://en.wikipedia.org/wiki/Magnetic_field" target="_blank">fields</a>.</p><p><a href="https://en.wikipedia.org/wiki/Ferromagnetic" target="_blank">Ferromagnetic</a> materials consist of <a href="https://en.wikipedia.org/wiki/Magnetic_domains" target="_blank">magnetic domains</a>. When a small external field �<img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/75a9edddcca2f782014371f75dca39d7e13a9c1b" alt="H" class="fr-fic fr-dii fr-draggable " style="" /> is applied, domains parallel to the external field start to grow. In this region, <a href="https://en.wikipedia.org/wiki/Domain_wall_(magnetism)" target="_blank">domain walls</a> are moving. They are hindered by material defects. <a href="https://en.wikipedia.org/wiki/Lord_Rayleigh" target="_blank">Lord Rayleigh</a> investigated this first <a href="https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-1" target="_blank">[1]</a> and quantified the magnetization �<img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/f82cade9898ced02fdd08712e5f0c0151758a0dd" alt="M" class="fr-fic fr-dii fr-draggable " style="" /> as a linear and quadratic term in the field:</p><p>�=�0�+���0�2.<img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/24d3008c08a989af93754d4a72ba2364b180bdd3" alt="M=\chi _{0}H+\alpha _{R}\mu _{0}H^{2}." class="fr-fic fr-dii fr-draggable " style="" /></p><p>Here �0<img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/ab65ab05ef061a305d53a395741e8dec6d267986" alt="\chi _{0}" class="fr-fic fr-dii fr-draggable " style="" /> is the initial <a href="https://en.wikipedia.org/wiki/Magnetic_susceptibility" target="_blank">susceptibility</a>, describing the reversible part of magnetisation reversal. The Rayleigh constant ��<img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/c0b59dabc51de8f86d4deb66c9f9d02f03864ba6" alt="\alpha_R" class="fr-fic fr-dii fr-draggable " style="" /> describes the irreversible <a href="https://en.wikipedia.org/wiki/Barkhausen_effect" target="_blank">Barkhausen jumps</a>.</p><p>The Rayleigh law was derived theoretically by <a href="https://en.wikipedia.org/wiki/Louis_N%C3%A9el" target="_blank">Louis Néel</a>.,<a href="https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-2" target="_blank">[2]</a><a href="https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-3" target="_blank">[3]</a></p><p>The same law describes polarization<a href="https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-4" target="_blank">[4]</a> and direct<a href="https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-5" target="_blank">[5]</a> and converse<a href="https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-6" target="_blank">[6]</a> <a href="https://en.wikipedia.org/wiki/Piezoelectric" target="_blank">piezoelectric</a> response of some <a href="https://en.wikipedia.org/wiki/Ferroelectric_material" target="_blank">ferroelectric</a> and ferroelectric-<a href="https://en.wikipedia.org/wiki/Ferroelastic" target="_blank">ferroelastic</a> materials. The common feature for ferromagnetic, ferroelectric and ferroelastic materials (i.e., <a href="https://en.wikipedia.org/wiki/Ferroic" target="_blank">ferroic</a> materials) are domains whose boundaries (domain walls) can be moved by magnetic, electric or mechanical fields.</p></blockquote><p></p>
[QUOTE="RichCoyle, post: 2886511, member: 127134"] Maybe you could translate that into hunter talk. [H1]Rayleigh law[/H1] 1 language From Wikipedia, the free encyclopedia [I]This article is about the magnetic law. For the stochastic distribution, see [URL='https://en.wikipedia.org/wiki/Rayleigh_distribution']Rayleigh distribution[/URL]. For optical scattering, see [URL='https://en.wikipedia.org/wiki/Rayleigh_scattering']Rayleigh scattering[/URL]. For wireless multipath propagation, see [URL='https://en.wikipedia.org/wiki/Rayleigh_fading']Rayleigh fading[/URL].[/I] The [B]Rayleigh law[/B] describes the behavior of [URL='https://en.wikipedia.org/wiki/Ferromagnetic']ferromagnetic[/URL] materials at low [URL='https://en.wikipedia.org/wiki/Magnetic_field']fields[/URL]. [URL='https://en.wikipedia.org/wiki/Ferromagnetic']Ferromagnetic[/URL] materials consist of [URL='https://en.wikipedia.org/wiki/Magnetic_domains']magnetic domains[/URL]. When a small external field �[IMG alt="H"]https://wikimedia.org/api/rest_v1/media/math/render/svg/75a9edddcca2f782014371f75dca39d7e13a9c1b[/IMG] is applied, domains parallel to the external field start to grow. In this region, [URL='https://en.wikipedia.org/wiki/Domain_wall_(magnetism)']domain walls[/URL] are moving. They are hindered by material defects. [URL='https://en.wikipedia.org/wiki/Lord_Rayleigh']Lord Rayleigh[/URL] investigated this first [URL='https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-1'][1][/URL] and quantified the magnetization �[IMG alt="M"]https://wikimedia.org/api/rest_v1/media/math/render/svg/f82cade9898ced02fdd08712e5f0c0151758a0dd[/IMG] as a linear and quadratic term in the field: �=�0�+���0�2.[IMG alt="M=\chi _{0}H+\alpha _{R}\mu _{0}H^{2}."]https://wikimedia.org/api/rest_v1/media/math/render/svg/24d3008c08a989af93754d4a72ba2364b180bdd3[/IMG] Here �0[IMG alt="\chi _{0}"]https://wikimedia.org/api/rest_v1/media/math/render/svg/ab65ab05ef061a305d53a395741e8dec6d267986[/IMG] is the initial [URL='https://en.wikipedia.org/wiki/Magnetic_susceptibility']susceptibility[/URL], describing the reversible part of magnetisation reversal. The Rayleigh constant ��[IMG alt="\alpha_R"]https://wikimedia.org/api/rest_v1/media/math/render/svg/c0b59dabc51de8f86d4deb66c9f9d02f03864ba6[/IMG] describes the irreversible [URL='https://en.wikipedia.org/wiki/Barkhausen_effect']Barkhausen jumps[/URL]. The Rayleigh law was derived theoretically by [URL='https://en.wikipedia.org/wiki/Louis_N%C3%A9el']Louis Néel[/URL].,[URL='https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-2'][2][/URL][URL='https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-3'][3][/URL] The same law describes polarization[URL='https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-4'][4][/URL] and direct[URL='https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-5'][5][/URL] and converse[URL='https://en.wikipedia.org/wiki/Rayleigh_law#cite_note-6'][6][/URL] [URL='https://en.wikipedia.org/wiki/Piezoelectric']piezoelectric[/URL] response of some [URL='https://en.wikipedia.org/wiki/Ferroelectric_material']ferroelectric[/URL] and ferroelectric-[URL='https://en.wikipedia.org/wiki/Ferroelastic']ferroelastic[/URL] materials. The common feature for ferromagnetic, ferroelectric and ferroelastic materials (i.e., [URL='https://en.wikipedia.org/wiki/Ferroic']ferroic[/URL] materials) are domains whose boundaries (domain walls) can be moved by magnetic, electric or mechanical fields. [/QUOTE]
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