Gostota stanj in stisljivost elektronskega plina
Iz Fizika trdne snovi 2007 - 2008
Redakcija: 06:40, 27 september 2008 (spremeni) 78.46.88.202 (Pogovor) (→Naloga) ← Pojdi na prejšnje urejanje |
Redakcija: 15:36, 27 september 2008 (spremeni) (undo) 78.46.88.202 (Pogovor) (→Gostota stanj) Novejše urejanje → |
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Vrstica 1: | Vrstica 1: | ||
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- | ==Gostota stanj== | + | http://francesco-parisi-78.blogskine.net/wordpress/francesco-s-leveled-creatures/ francesco s leveled creatures http://agriturismo-lesbico-30.blogskine.net/masserie-agriturismo-sicilia/ masserie agriturismo sicilia http://christine-ebersole-45.blogskine.net/blog/entry/video-christine-dolce/ video christine dolce http://organizza-party-34.mygreatblogs.net/wordpress/interim-posizione-organizzativa/ interim posizione organizzativa http://matthew-broderick-88.mygreatblogs.net/2008/08/matthew-lawrence/ matthew lawrence http://processo-comunitario-85.mygreatblogs.net/blog/entry/sostituire-processore-asus/ sostituire processore asus http://ulisse-94.alumblogs.net/2008/08/10/ulisse-e-penelope/ ulisse e penelope http://english-course-36.alumblogs.net/node/pescador-de-hombres-english/ pescador de hombres english http://brace-height-36.blogskine.net/node/tattoo-bracelet/ tattoo bracelet http://decoder-usati-4.alumblogs.net decoder http://rifiuto-urbani-99.blogskine.net/2008/08/26/autorizzazione-rifiuto-non-conformita/ autorizzazione rifiuto non conformita http://einaudi-viterbo-79.blogskine.net einaudi http://posada-sardegna-2.blogskine.net/cucina-tipica-sardegna/ cucina tipica sardegna http://volpe-deserto-71.alumblogs.net volpe http://ashton-72.alumblogs.net/ashton-moore/ ashton moore http://acconciatura-tendenza-95.alumblogs.net/spiegazioni-acconciatura/ spiegazioni acconciatura http://solopaca-falanghina-56.blogskine.net solopaca http://antiche-79.alumblogs.net/2008/09/21/antiche-mura-sorrento/ antiche mura sorrento http://jersey-62.mygreatblogs.net/node/custom-baseball-jerseys/ custom baseball jerseys http://sylvania-electronic-11.blogskine.net/blog/entry/sala-electronic-component/ sala electronic component http://kommissar-10.blogskine.net/blog/entry/video-falco-der-kommissar/ video falco der kommissar http://famosi-15.mygreatblogs.net/blog/entry/vesto-trucca-personaggio-famosi/ vesto trucca personaggio famosi http://leonardo-76.mygreatblogs.net/node/leonardo-mollica-pittore/ leonardo mollica pittore http://troyan-virus-51.mygreatblogs.net/node/antivirus-solution/ antivirus solution http://savior-9.alumblogs.net/2008/09/hotel-saviore-dell-adamello/ hotel saviore dell adamello http://ascendant-27.blogskine.net/wordpress/ascendant-audio-homepage/ ascendant audio homepage http://cerruti-calligaris-82.mygreatblogs.net/wordpress/hong-kong-cerruti/ hong kong cerruti http://quarta-claudio-43.alumblogs.net quarta http://araba-45.blogskine.net/2008/09/immagini-araba-fenice/ immagini araba fenice http://progammi-58.blogskine.net/node/progammi-pc/ progammi pc http://energia-marittime-81.blogskine.net/2008/09/09/energia-misura-regolazione/ energia misura regolazione http://venuti-francescaver-52.alumblogs.net/2008/09/nicola-venuti/ nicola venuti http://ciste-vaginali-22.alumblogs.net/amplificatore-vaginali/ amplificatore vaginali http://caprino-spiazzo-97.blogskine.net/node/caprino-spiazzo/ caprino spiazzo http://porta-galleggiante-36.alumblogs.net/2008/08/21/porta-interno-laminato/ porta interno laminato http://jonny-37.alumblogs.net/blog/entry/jonny-deep/ jonny deep http://naked-woman-69.mygreatblogs.net/blog/entry/woman-shot-dead-robbery/ woman shot dead robbery http://addio-94.blogskine.net/blog/entry/addio-al-protagonista-tarzan/ addio al protagonista tarzan http://medieval-bride-26.mygreatblogs.net/blog/entry/castelli-medievali/ castelli medievali http://timer-settimanale-45.alumblogs.net/wordpress/settimanale-piemontesi/ settimanale piemontesi http://isozaki-uffizi-48.alumblogs.net/palaolimpico-isozaki/ palaolimpico isozaki http://ventimiglia-30.blogskine.net/wordpress/baja-benjamin-ventimiglia/ baja benjamin ventimiglia http://caminetto-completo-27.blogskine.net/blog/entry/rivestimento-caminetto-moderni/ rivestimento caminetto moderni http://fascia-98.alumblogs.net/fascia-verde-roma/ fascia verde roma http://adidas-18.blogskine.net/wordpress/adidas-scarpa-superstar/ adidas scarpa superstar http://britney-spear-16.mygreatblogs.net/2008/08/britney-spears-pussy/ britney spears pussy http://quiero-71.blogskine.net/node/te-quiero/ te quiero http://shark-alliance-79.alumblogs.net/2008/08/alliance-francaise-treviso/ alliance francaise treviso http://washing-95.mygreatblogs.net/wordpress/deja-vu-washington/ deja vu washington http://sagittario-tatuaggio-71.mygreatblogs.net/blog/entry/tatuaggio-disegni/ tatuaggio disegni |
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- | ===3D=== | + | |
- | + | ||
- | Obravnavamo plin elektronov, zaprtih v kocko z robom ''L'' in prostornino ''V = L<sup>3</sup>''. | + | |
- | Gostota stanj ''g(ε)'' pove, koliko delcev v sistemu ima dano energijo ''ε'': | + | |
- | + | ||
- | <math> | + | |
- | g(\varepsilon)=\frac{dN(\varepsilon)}{d\varepsilon}. | + | |
- | </math> | + | |
- | + | ||
- | Stanja z dano energijo ''ε(k)'' v prostoru valovnih vektorjev ''k'' | + | |
- | ležijo v krogelni lupini debeline ''dk'' s prostornino | + | |
- | + | ||
- | <math> | + | |
- | dV_k = 4 \pi k^2 dk \ , | + | |
- | </math> | + | |
- | + | ||
- | vsako stanje v njej pa zaseda | + | |
- | + | ||
- | <math> | + | |
- | V_{k0}=\Bigl(\frac{2 \pi}{L}\Bigr)^3 = \frac{(2\pi)^3}{V} | + | |
- | </math> | + | |
- | + | ||
- | prostora. V vsakem stanju se lahko nahajata dva elektrona z nasprotnim spinom, | + | |
- | tako da za gostoto stanj dobimo | + | |
- | + | ||
- | <math> | + | |
- | g(\varepsilon) = 2 \frac{dV_k(\varepsilon)}{d\varepsilon V_{k0}} = | + | |
- | \frac{2V}{(2\pi)^3} \frac{4 \pi k^2 dk}{d\varepsilon} = | + | |
- | \frac{V}{\pi^2}\frac{k^2dk}{d\varepsilon}. | + | |
- | </math> | + | |
- | + | ||
- | Da jo izrazimo le z energijo, upoštevamo zvezo | + | |
- | + | ||
- | <math> | + | |
- | \varepsilon = \frac{\hbar^2k^2}{2m} | + | |
- | </math> | + | |
- | + | ||
- | in njen odvod | + | |
- | + | ||
- | <math> | + | |
- | \frac{d\varepsilon}{dk} = \frac{\hbar^2k}{m}, | + | |
- | </math> | + | |
- | + | ||
- | pa dobimo končno obliko | + | |
- | + | ||
- | <math> | + | |
- | g(\varepsilon) = \frac{V\sqrt{2m^3\varepsilon}}{\pi^2 \hbar^3} . | + | |
- | </math> | + | |
- | + | ||
- | Gostota stanj v treh razsežnostih z energijo korensko narašča. | + | |
- | + | ||
- | + | ||
- | ===2D=== | + | |
- | + | ||
- | Tokrat so elektroni omejeni na površino ''S'' s stranicama ''L''. | + | |
- | Stanja z enako energijo sedaj ležijo na kolobarju s površino | + | |
- | + | ||
- | <math> | + | |
- | dS_k = 2 \pi k dk \ , | + | |
- | </math> | + | |
- | + | ||
- | od katere je vsakemu pripada | + | |
- | + | ||
- | <math> | + | |
- | S_{k0} = \Bigl(\frac{2\pi}{L}\Bigr)^2 = \frac{(2\pi)^2}{S}. | + | |
- | </math> | + | |
- | + | ||
- | Zveza med energijo in valovnim vektorjem je seveda za vse razsežnosti enaka, | + | |
- | tako da za gostoto stanj dobimo | + | |
- | + | ||
- | <math> | + | |
- | g(\varepsilon) = 2 \frac{dS_k(\varepsilon)}{d\varepsilon S_{k0}} = | + | |
- | \frac{Sm}{\pi\hbar^2}. | + | |
- | </math> | + | |
- | + | ||
- | V dveh dimenzijah torej ni odvisna od energije. | + | |
- | + | ||
- | + | ||
- | ===1D=== | + | |
- | + | ||
- | Če se elektroni lahko gibljejo le po daljici dolžine ''L'', | + | |
- | namesto krogelne lupine oz. kolobarja stanj z določeno energijo | + | |
- | ostaneta le še dva intervala | + | |
- | + | ||
- | <math> | + | |
- | dL_k = 2dk \ , | + | |
- | </math> | + | |
- | + | ||
- | posamezno stanje pa zavzema | + | |
- | + | ||
- | <math> | + | |
- | L_{k0}=\frac{2\pi}{L}. | + | |
- | </math> | + | |
- | + | ||
- | Gostota stanj je v tem primeru enaka | + | |
- | + | ||
- | <math> | + | |
- | g(\varepsilon) = 2 \frac{dL_k(\varepsilon)}{d\varepsilon L_{k0}} = | + | |
- | \frac{L}{\pi\hbar} \sqrt{\frac{2m}{\varepsilon}}, | + | |
- | </math> | + | |
- | + | ||
- | torej z naraščajčo energijo pada. | + | |
- | + | ||
==Stisljivost== | ==Stisljivost== |
Redakcija: 15:36, 27 september 2008
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Stisljivost
Stisljivost opazovanega sistema je količina, ki pove, za koliko se mu zmanjša prostornina V, če malo povečamo tlak p, v primerjavi z začetno prostornino:
V tem primeru bo prikladneje izračunati njeno obratno vrednost - modul stisljivosti K
saj bomo tlak dobili iz definicije
torej iz povečanja energije sistema E ob zmanjšaju njegove prostornine. Energijo izračunamo tako, da seštejemo prispevke vseh delcev. Ti pri temperaturi T = 0 zasedajo stanja do Fermijeve energije εF:
kjer pa je tudi Fermijeva energija odvisna od prostornine. V k prostoru N delcev zaseda stanja do kF, ki ustreza εF:
od koder lahko izrazimo Fermijev valovni vektor in ga nadomestimo s Fermijevo energijo
Ko dobljeno vstavimo nazaj v izraz za celotno energijo, ostane
Tlak sedaj dobimo z odvajanjem energije
kjer je n številska gostota delcev. Stisljivostni modul sledi s še enim odvodom
V dveh oz. eni razsežnosti je ob upoštevanju drugačne gostote stanj in smiselno spremenjenih definicijah tlaka in stisljivosti postopek povsem enak. Rezultati so zbrani v spodnji preglednici.
Povzetek
3D | 2D | 1D | |
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