{"id":7629,"date":"2021-11-17T14:06:22","date_gmt":"2021-11-17T11:06:22","guid":{"rendered":"https:\/\/bestessayhomework.com\/tr\/?p=7629"},"modified":"2021-11-17T14:06:22","modified_gmt":"2021-11-17T11:06:22","slug":"katmanli-bolge-modeli-is-sagligi-ve-guvenligi-tez-yaptirma-isg-is-sagligi-ve-guvenligi-tez-yaptirma-ucretleri","status":"publish","type":"post","link":"https:\/\/bestessayhomework.com\/tr\/katmanli-bolge-modeli-is-sagligi-ve-guvenligi-tez-yaptirma-isg-is-sagligi-ve-guvenligi-tez-yaptirma-ucretleri\/","title":{"rendered":"KATMANLI B\u00d6LGE MODEL\u0130 \u2013 \u0130\u015f Sa\u011fl\u0131\u011f\u0131 ve G\u00fcvenli\u011fi Tez Yapt\u0131rma \u2013 \u0130SG \u2013 \u0130\u015f Sa\u011fl\u0131\u011f\u0131 ve G\u00fcvenli\u011fi Tez Yapt\u0131rma \u00dccretleri"},"content":{"rendered":"

D\u0130KEY KONSANTRASYON PROF\u0130LLER\u0130NE SAH\u0130P <\/span><\/strong><\/h3>\n

KATMANLI B\u00d6LGE MODEL\u0130<\/span><\/strong><\/h3>\n

Tamanini ve Chaffe (2000), zemin seviyesinde nazik\u00e7e sal\u0131nan s\u0131v\u0131 propanla yap\u0131lan deneylerden, propanda belirli bir y\u00fcksekli\u011fe kadar dikey konsantrasyonlar\u0131n geli\u015fti\u011fini buldu. Propan\u0131n konsantrasyonu dikey olarak azald\u0131k\u00e7a, propan\/hava kar\u0131\u015f\u0131m\u0131n\u0131n yo\u011funlu\u011fu, pc(z) de dikey olarak azald\u0131.<\/span><\/p>\n

Propan\/hava \u00f6zg\u00fcl a\u011f\u0131rl\u0131\u011f\u0131, SCmin veya e\u015fik yo\u011funlu\u011fu Pcmin’e kar\u015f\u0131l\u0131k gelen belirli bir y\u00fckseklikte, bu noktan\u0131n \u00fczerindeki konsantrasyonlar esasen mol fraksiyonu, YCmix ve yo\u011funluk ~12mix ile iyi kar\u0131\u015f\u0131r hale geldi.<\/span>\u00a0\u0130ki b\u00f6lgeli WELMIX modelini genelle\u015ftirin ve a\u015fa\u011f\u0131da tan\u0131mland\u0131\u011f\u0131 gibi \u00fc\u00e7 b\u00f6lgeli bir model \u00f6nerin. T\u00fcm yan\u0131c\u0131 buharlar\u0131n i\u00e7eri girmesi i\u00e7in yak\u0131t buharlar\u0131n\u0131n hi\u00e7 olmad\u0131\u011f\u0131 veya d\u00fc\u015f\u00fck yo\u011funlukta oldu\u011fu bir \u00fcst b\u00f6lgeye (so\u011fuk b\u00f6lge) sahip olmak, sonraki patlama modelimiz i\u00e7in faydal\u0131 oldu\u011funu kan\u0131tl\u0131yor.<\/span><\/p>\n

Alttaki iki b\u00f6lge, WELMIX modelindeki kar\u0131\u015f\u0131k b\u00f6lgenin yerini al\u0131r ve a\u015fa\u011f\u0131daki yanma modelinde birlikte s\u0131cak gazlar\u0131n b\u00f6lgesini olu\u015fturur.<\/span><\/p>\n

Tamanini ve Chaffe, tabakal\u0131 ve kar\u0131\u015f\u0131k b\u00f6lgeler aras\u0131ndaki yo\u011funluk e\u015fi\u011fi i\u00e7in bir korelasyon sunmak veya dikey konsantrasyon profilini tan\u0131mlayan bir ifade sunmak i\u00e7in yeterli veriye sahip de\u011fildi. Kesin verilerin yoklu\u011funda, Tamanini ve Chaffe’nin deneylerinde a\u00e7\u0131klanan \u00f6zellikleri sa\u011flayan ve gerekli katsay\u0131lar\u0131n de\u011ferlerinin gelecekte iyile\u015ftirilmesine izin veren bir \u00e7er\u00e7eve \u00f6neriyoruz. Dikey konsantrasyon profilleri i\u00e7in yayg\u0131n olarak kabul edilen bir form olan Gauss profili, ama\u00e7lar\u0131m\u0131z i\u00e7in yeterlidir.<\/span><\/p>\n

Tabakala\u015fman\u0131n bitti\u011fi ve karma b\u00f6lgenin ba\u015flad\u0131\u011f\u0131 dikey y\u00fckseklik, Zmix, kar\u015f\u0131l\u0131k gelen \u00f6zg\u00fcl a\u011f\u0131rl\u0131k profilinden bulunur. \u015eekil 2 parseller Denk. 8, yc(z)\/yc~ olarak, tabakala\u015fma tabakas\u0131 1-3 m’den daha az derinlikte ise de\u011ferlerinin birlik mertebesinde olabilece\u011fini g\u00f6sterir. Zmix’i bularak, B\u00f6lge 1’in hacmini V1, tabakal\u0131 b\u00f6lge tan\u0131mlar\u0131z ve ayr\u0131ca yeni bir kar\u015f\u0131l\u0131k gelen hacim fraksiyonlar\u0131 seti tan\u0131mlar\u0131z, q l , q 2 , q3.<\/span><\/p>\n

Bir ba\u015fka genelleme olarak, modelimiz, a\u015f\u0131r\u0131 \u0131s\u0131t\u0131lm\u0131\u015f bir s\u0131v\u0131n\u0131n de\u015farj \u00fczerine ilk yan\u0131p s\u00f6nmesinden ve zemine d\u00fc\u015fmeden veya bir havuz olu\u015fturmak i\u00e7in “ya\u011fmurdan” \u00f6nce buharla\u015fan aerosol damlalar\u0131ndan ek buhar kaynaklar\u0131na izin verir. Bu katk\u0131lar do\u011frusal olarak toplamsal olarak ele al\u0131nabilir, bu nedenle a\u015fa\u011f\u0131daki tart\u0131\u015fmay\u0131 onlar\u0131 dahil ederek karma\u015f\u0131kla\u015ft\u0131rm\u0131yoruz, ancak bunlar kodlanm\u0131\u015f modelde ele al\u0131nm\u0131\u015ft\u0131r.<\/span><\/p>\n

1. ve 2. B\u00f6lgeler Aras\u0131nda K\u00fctleyi Da\u011f\u0131tma<\/span><\/strong><\/h3>\n

Alt iki b\u00f6lgedeki kirletici k\u00fctlesi, WELMIX model tahminlerinden her zaman ad\u0131m\u0131nda bilinir. Tabakal\u0131 b\u00f6lge modeli ile \u00f6nce B\u00f6lge 1’in s\u0131n\u0131rlar\u0131n\u0131 tan\u0131ml\u0131yoruz ve ard\u0131ndan b\u00f6lgedeki toplam k\u00fctleyi bulmak i\u00e7in konsantrasyon profilini entegre ediyoruz. Fark olarak, B\u00f6lge 2’deki kirleticinin hacmini ve k\u00fctlesini buluyoruz. Daha sonra B\u00f6lge 1 ve 2 i\u00e7in yan\u0131c\u0131 k\u00fctle bulunur ve e\u011fer hakl\u0131ysa, yanma modeli i\u00e7in toplam yan\u0131c\u0131 k\u00fctleyi elde etmek i\u00e7in eklenir.<\/span><\/p>\n

B\u00f6lge 1, mT1’deki toplam k\u00fctleyi bulmak i\u00e7in toplam yo\u011funluk profilini ayn\u0131 s\u0131n\u0131rlar \u00fczerinde entegre edin. Bu entegrasyon i\u00e7in yo\u011funlu\u011fu bulmak i\u00e7in adyabatik kar\u0131\u015ft\u0131rma rutini taraf\u0131ndan geli\u015ftirilen yak\u0131t\u0131n toplam yo\u011funluk ve mol fraksiyonu \u00e7iftlerini enterpolasyon yap\u0131n. B\u00f6lge 1’deki ortalama k\u00fctle oran\u0131na bak\u0131l\u0131r.<\/span><\/p>\n

\n

OSI modeli<\/a><\/span>
\nOSI uygulama katman\u0131<\/span>
\nOSI Katmanlar\u0131 PDF<\/span>
\nUygulama katman\u0131 protokolleri<\/span>
\nOsi Nedir<\/span>
\nBilgisayar a\u011flar\u0131n\u0131n katmanl\u0131 yap\u0131s\u0131<\/span>
\ny\u00f6nlendirici (router) osi referans modelinin hangi katman\u0131nda \u00e7al\u0131\u015f\u0131r<\/span>
\nFiziksel katman protokolleri<\/span><\/p>\n

\n

Odan\u0131n s\u0131cak ve so\u011fuk b\u00f6l\u00fcmlerindeki ilk k\u00fctle, hacim ve yo\u011funluk B\u00f6l\u00fcm 4’ten bilinmektedir. Bundan sonra 1, 2, 3 alt simgeleri, a\u015fa\u011f\u0131daki a\u015famalardaki termodinamik durumlara at\u0131fta bulunacakt\u0131r: ilk (l), yanma ( 2), geni\u015fleme s\u0131k\u0131\u015ft\u0131rma (3). S\u0131cak b\u00f6lge, ortam bas\u0131nc\u0131 Phl’Pamb’da ve ortalama s\u0131cakl\u0131kta Thl’de, yine adyabatik kar\u0131\u015ft\u0131rma tablosundan enterpolasyonla bulunan bir Vhl ba\u015flang\u0131\u00e7 \u200b\u200bhacmine sahiptir.<\/span><\/p>\n

S\u0131cak b\u00f6lge, Th3 ve Ph3 son durumuna geni\u015fledik\u00e7e, so\u011fuk b\u00f6lgedeki k\u00fctleyi s\u0131k\u0131\u015ft\u0131r\u0131r. So\u011fuk b\u00f6lge ba\u015flang\u0131\u00e7ta, ortam s\u0131cakl\u0131\u011f\u0131nda Tcl=Tamb ve Pcl=Pamb bas\u0131nc\u0131nda Vcl=V3 hacmindedir ve Tc3 ve Pc3 son durumuna s\u0131k\u0131\u015ft\u0131r\u0131l\u0131r. Her iki b\u00f6lgedeki nihai bas\u0131n\u00e7 e\u015fit olmal\u0131 ve nihai hacimler Vh3 ve Vc3’\u00fcn toplam\u0131 toplam oda hacmine e\u015fit olmal\u0131d\u0131r.<\/span><\/p>\n

S\u0131cak taraftaki yanma, iki alternatif varsay\u0131mdan biri kullan\u0131larak iki ad\u0131mda hesaplan\u0131r.<\/span><\/p>\n

\u0130zobarik Se\u00e7enek<\/span><\/strong><\/h3>\n

1) Yan\u0131c\u0131 hacim vh =qhv’yi sabit, ortam bas\u0131nc\u0131nda, PI, ara s\u0131cak taraf s\u0131cakl\u0131\u011f\u0131na, Th2’ye yak\u0131n.<\/span>
\n2) Yan\u0131c\u0131 hacmi sabit hacimde ara s\u0131cak taraf s\u0131cakl\u0131\u011f\u0131, Th2 ve bas\u0131n\u00e7, Ph2’ye kadar yak\u0131n. S\u0131cak gazlar\u0131 sabit hacimde, Ph2’de tutmak i\u00e7in gereken bas\u0131nc\u0131 hesaplay\u0131n.<\/span><\/p>\n

Her iki durumda da s\u0131cak yan yanma \u00fcr\u00fcnlerinin ortalama molek\u00fcler a\u011f\u0131rl\u0131\u011f\u0131n\u0131, Mh2’yi buluyoruz. Her iki durumda da ikinci ad\u0131m, s\u0131cak b\u00f6lgenin adyabatik geni\u015flemesi ve so\u011fuk b\u00f6lgenin adyabatik s\u0131k\u0131\u015ft\u0131r\u0131lmas\u0131d\u0131r. Bu durumlar\u0131 a\u00e7\u0131klayan denklemler a\u015fa\u011f\u0131da a\u00e7\u0131klanm\u0131\u015ft\u0131r.<\/span><\/p>\n

Durum 2, Yanma \u00dcr\u00fcnleri, \u0130zobarik \u00c7\u00f6z\u00fcm<\/span><\/strong><\/p>\n

Sabit bas\u0131n\u00e7ta yanmadan sonra, adyabatik alev s\u0131cakl\u0131k mod\u00fcl\u00fc, yanma \u00fcr\u00fcnleri olan Th2 ve Mh2’nin s\u0131cakl\u0131\u011f\u0131n\u0131 ve molek\u00fcler a\u011f\u0131rl\u0131\u011f\u0131n\u0131 sa\u011flar. K\u00fctleyi koruyarak ve ideal gaz yo\u011funlu\u011funu kullanarak s\u0131cak taraf hacmini, Vh2’yi verir. Bu hacim, mevcut hacimden daha b\u00fcy\u00fck olabilir. Bu ger\u00e7ek\u00e7i olmayan durum, Durum 3’te d\u00fczeltilmi\u015ftir.<\/span><\/p>\n

Durum 3, S\u0131k\u0131\u015ft\u0131r\u0131lm\u0131\u015f Ko\u015fullar, \u0130zobarik \u00c7\u00f6z\u00fcm<\/span><\/strong><\/p>\n

Yand\u0131ktan sonra, s\u0131cak taraf geni\u015fleyecek ve so\u011fuk taraf\u0131 s\u0131k\u0131\u015ft\u0131racak ve yeni bir hacim fraksiyonu, Th3 elde edecektir. Her iki tarafta k\u00fctle korundu\u011fu i\u00e7in, yeni yo\u011funluklar vard\u0131r.<\/span><\/p>\n

Benzer \u015fekilde, yc, TIto Tc3 s\u0131cakl\u0131\u011f\u0131 \u00fczerinden ortalamas\u0131 al\u0131nan so\u011fuk taraftaki malzeme (\u00e7o\u011funlukla hava) i\u00e7in \u00f6zg\u00fcl \u0131s\u0131 oran\u0131d\u0131r. Th2’den Th3’\u00fc bulmada kullan\u0131lan yo\u011funluk, s\u0131cak taraf\u0131n geni\u015flemesi vh hacminden ba\u015flad\u0131\u011f\u0131 i\u00e7in ba\u015flang\u0131\u00e7 \u200b\u200byo\u011funlu\u011fu, P h i’dir. Son bas\u0131n\u00e7, P3, hem s\u0131cak hem de so\u011fuk taraflar i\u00e7in ayn\u0131 olmal\u0131d\u0131r. Durum 3’teki denklemler, yaln\u0131zca tek bir bilinmeyenin,7h3’\u00fcn bir fonksiyonudur, bu nedenle denklemin k\u00f6k\u00fcn\u00fc bulma sorunudur.<\/span><\/p>\n

Bu, bir k\u00f6k bulma algoritmas\u0131 kullan\u0131larak kolayca yap\u0131l\u0131r. Problemin her zaman yak\u0131nsad\u0131\u011f\u0131, izobarik \u00e7\u00f6z\u00fcm i\u00e7in \u015eekil 3’te g\u00f6sterilmektedir. Yani, artan q h3 ile s\u0131cak taraf\u0131n bas\u0131nc\u0131 azal\u0131r ve so\u011fuk taraf\u0131n bas\u0131nc\u0131 artar.<\/span><\/p>\n

\u0130ki \u00e7\u00f6z\u00fcm aras\u0131ndaki tek fark, izokorik \u00e7\u00f6z\u00fcm i\u00e7in ara bas\u0131nc\u0131n Denklem’den al\u0131nmas\u0131d\u0131r. 22b. Geni\u015fleme s\u0131k\u0131\u015ft\u0131rma form\u00fcllerinden izokorik \u00e7\u00f6zelti i\u00e7in analitik bir yakla\u015f\u0131m elde edilir.<\/span><\/p>\n","protected":false},"excerpt":{"rendered":"

D\u0130KEY KONSANTRASYON PROF\u0130LLER\u0130NE SAH\u0130P KATMANLI B\u00d6LGE MODEL\u0130 Tamanini ve Chaffe (2000), zemin seviyesinde nazik\u00e7e sal\u0131nan s\u0131v\u0131 propanla yap\u0131lan deneylerden, propanda belirli bir y\u00fcksekli\u011fe kadar dikey konsantrasyonlar\u0131n geli\u015fti\u011fini buldu. Propan\u0131n konsantrasyonu dikey olarak azald\u0131k\u00e7a, propan\/hava kar\u0131\u015f\u0131m\u0131n\u0131n yo\u011funlu\u011fu, pc(z) de dikey olarak azald\u0131. Propan\/hava \u00f6zg\u00fcl a\u011f\u0131rl\u0131\u011f\u0131, SCmin veya e\u015fik yo\u011funlu\u011fu Pcmin’e kar\u015f\u0131l\u0131k gelen belirli bir y\u00fckseklikte, bu…
Devam\u0131<\/a><\/p>\n","protected":false},"author":6,"featured_media":6944,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"om_disable_all_campaigns":false,"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"categories":[16538,16536,16540,16539,16537],"tags":[16545,16547,16543,16541,16544,16542,16546],"class_list":["post-7629","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-bilgisayar-aglarinin-katmanli-yapisi","category-fiziksel-katman-protokolleri","category-osi-modeli","category-uygulama-katmani-protokolleri","category-yonlendirici-router-osi-referans-modelinin-hangi-katmaninda-calisir","tag-bilgisayar-aglarinin-katmanli-yapisi","tag-fiziksel-katman-protokolleri","tag-osi-katmanlari-pdf-uygulama-katmani-protokolleri","tag-osi-modeli","tag-osi-nedir","tag-osi-uygulama-katmani","tag-yonlendirici-router-osi-referans-modelinin-hangi-katmaninda-calisir"],"aioseo_notices":[],"aioseo_head":"\n\t\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t\n\t\t