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An gudanar da gwaje-gwaje a cikin tashar rectangular da aka katange ta hanyar layi na nau'i-nau'i na nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i nau'i). d wanda ke danganta matsa lamba a wurare masu mahimmanci na tsarin zuwa halayen halayen sanda. An samo ka'idar 'yancin kai don riƙe mafi yawan lambobin Euler da ke nuna matsa lamba a wurare daban-daban, watau idan matsa lamba ba shi da girma ta amfani da tsinkaya na saurin shigar da ke al'ada ga sanda, saitin ya kasance mai zaman kanta daga kusurwar tsoma.Za'a iya amfani da alaƙar da aka samu na ɗan lokaci don Zane irin na'urorin lantarki.
Mutane da yawa zafi da taro canja wurin na'urorin kunshi wani sa na kayayyaki, tashoshi ko Kwayoyin ta hanyar abin da ruwaye wucewa a cikin fiye ko žasa hadaddun ciki Tsarin kamar sanduna, buffers, abun da ake sakawa, da dai sauransu.More kwanan nan, akwai an sabunta sha'awa a samun mafi fahimtar hanyoyin da alaka da ciki matsa lamba rarraba da kuma sojojin a kan hadaddun internals zuwa ga overall matsa lamba drop na the general matsa lamba na module.Among da sauran abubuwa, da kimiyya ta fadada man fetur module.Among da sauran abubuwa, da kimiyya da aka fadada man fetur da compilities. mulations, da kuma ƙara miniaturization na na'urorin.Recent gwaji karatu na matsa lamba na ciki rarraba da kuma asarar sun hada da tashoshi roughened da daban-daban siffa hakarkarinsa 1 , electrochemical reactor Kwayoyin 2 , capillary constriction 3 da lattice frame kayan 4 .
Mafi yawan tsarin da aka fi sani da ciki shine igiyoyin cylindrical ta hanyar naúrar naúrar, ko dai daure ko ware.A cikin masu musayar zafi, wannan tsari yana da mahimmanci a kan gefen harsashi.Shell gefen matsa lamba yana da alaƙa da zane na masu musayar zafi kamar masu samar da tururi, condensers da evaporators.A cikin binciken kwanan nan, Wang et al.5 samu reattachment da co-detachment kwarara jihohin a cikin wani tandem sanyi na sanduna.Liu et al.6 auna matsa lamba digo a cikin rectangular tashoshi tare da gina-in biyu U-dimbin yawa tube daure tare da daban-daban karkata kusurwoyi da calibrated wani lambobi model simulating sanda daure tare da porous kafofin watsa labarai.
Kamar yadda aka sa ran, akwai wasu nau'o'in daidaitawa waɗanda ke shafar aikin hydraulic na banki na silinda: nau'in tsari (misali, maɗaukaki ko cikin layi), ma'auni na dangi (misali, farar, diamita, tsayi), da kusurwar karkata, da sauransu.Mawallafa da yawa sun mayar da hankali kan gano ma'auni marasa girma don shiryar da zane-zane don kama abubuwan da suka haɗa da sigogi na geometric.A cikin binciken gwaji na baya-bayan nan, Kim et al.7 ya ba da shawarar ingantaccen samfurin porosity ta amfani da tsawon naúrar tantanin halitta azaman ma'aunin sarrafawa, ta yin amfani da tandem da tsattsauran ra'ayi da lambobi na Reynolds tsakanin 103 da 104.Snarski8 yayi nazarin yadda bakan wutar lantarki, daga accelerometers da wayoyin hydrophones da aka haɗe zuwa silinda a cikin rami na ruwa, ya bambanta tare da karkatar da jagorar kwarara et al.9 yayi nazarin rarraba matsa lamba na bango a kusa da sandar cylindrical a cikin yaw airflow.Mityakov et al.10 ya tsara filin saurin gudu bayan silinda yawed ta amfani da sitiriyo PIV.Alam et al.11 ya gudanar da wani cikakken nazari na tandem cylinders, mayar da hankali kan sakamakon Reynolds lambar da geometric rabo a kan vortex zubar.Sun iya gane biyar jihohi, wato kulle, intermittent kulle, babu kullewa, subharmonic kulle da kara Layer reattachment jihohin. Kwanan lambobi karatu sun nuna zuwa ga samuwar ta hanyar vortex tsarin ya kwarara.
Gabaɗaya, ana sa ran aikin hydraulic na tantanin halitta zai dogara ne akan tsari da lissafi na tsarin ciki, yawanci ana ƙididdige su ta hanyar alaƙar alaƙa na takamaiman ma'aunin gwaji. .A misali misali ne fitarwa equation ga wani orifice farantin 15.A cikin musamman hali na karkata sanduna, ko a cikin tsare ko bude kwarara, wani ban sha'awa ma'auni sau da yawa kawo a cikin wallafe-wallafe da kuma amfani da zanen kaya shi ne rinjaye na'ura mai aiki da karfin ruwa girma (misali, matsa lamba drop, karfi, vortex zubar mita, da dai sauransu) ) to lamba .) to da ma'auni mai ban sha'awa sau da yawa aka ambata a cikin wallafe-wallafen da kuma amfani da zanen kaya shi ne rinjaye na'ura mai aiki da karfin ruwa girma (misali, matsa lamba drop, karfi, vortex zubar mita, da dai sauransu) ) to lamba.) zuwa ga kwarara zuwa ga ka'idar ta kowane lokaci. Ana haifar da haɓakawa da farko ta hanyar shigar da al'ada na al'ada da kuma cewa tasirin axial wanda ke daidaitawa tare da axis na Silinda ba shi da kyau.Ko da yake babu wata yarjejeniya a cikin wallafe-wallafen game da ƙimar ingancin wannan ma'auni, a yawancin lokuta yana ba da ƙididdiga masu amfani a cikin rashin tabbas na gwaji na hali na empirical empirical . g417.
A cikin aikin da ake yi yanzu, an gabatar da sakamakon binciken binciken matsa lamba na ciki da raguwar matsa lamba a cikin tashar tare da layin madaidaiciya na sandunan cylindrical hudu masu karkata. Auna majalissar sanda guda uku tare da diamita daban-daban, canza kusurwar ni'ima. Manufar gabaɗaya ita ce bincikar hanyar ta hanyar abin da rarrabawar matsa lamba akan sandar sandar ke da alaƙa da juzu'in matsin lamba na cylindrical guda huɗu da aka yi amfani da shi ta hanyar bincikar ƙa'idar Berupeupe. na ƙarfin hali don kimanta ingancin ƙa'idar 'yancin kai. A ƙarshe, ana haifar da haɗin kai mara nauyi wanda za'a iya amfani dashi don tsara irin na'urorin hydraulic.
Saitin gwajin ya ƙunshi sashin gwaji na rectangular wanda ya karɓi kwararar iska da aka bayar ta hanyar axial fan. Sashen gwajin ya ƙunshi naúrar da ke kunshe da sandunan tsakiya guda biyu masu daidaituwa da rabi-biyu da aka saka a cikin bangon tashar, kamar yadda aka nuna a cikin 1e.
Sashin shigarwa (tsawon tsayi a mm) .Ƙirƙiri b ta amfani da Openscad 2021.01, openscad.org.Babban gwajin sashen (tsawon tsayi a mm) .An ƙirƙira shi tare da Opencad 2021.01, openscad.org c Ra'ayi mai zurfi na babban ɓangaren gwajin (tsawon mm) .An ƙirƙira ta amfani da Opencad 2021.01 tare da buɗewa mmcadle 2021.01. 1.01, fashe fashe na sashin gwaje-gwaje na openscad.org e.An ƙirƙira tare da Opencad 2021.01, openscad.org.
An gwada nau'i uku na sanduna na diamita daban-daban. Table 1 ya lissafa halaye na geometrical na kowane akwati. Ana ɗora sandunan a kan wani protractor don haka kusurwar su dangane da jagorancin gudana zai iya bambanta tsakanin 90 ° da 30 ° (Figures 1b da 3) . Dukkanin sanduna an yi su ne da bakin karfe kuma an yi su a tsakiya don kula da matsayi guda biyu a waje da gars da ke kusa da wurin da ke kusa da sararin samaniya. .
An auna ma'auni na shigarwa na sashin gwajin ta hanyar calibrated venturi, kamar yadda aka nuna a cikin Hoto 2, kuma ana kula da shi ta amfani da DP Cell Honeywell SCX. An auna yawan zafin jiki na ruwa a ma'auni na sashin gwajin tare da ma'aunin ma'aunin zafi da sanyio na PT100 kuma ana sarrafa shi a 45 ± 1 ° C. Don tabbatar da rarraba saurin tsarin tsari da kuma rage matakin da aka yi ta hanyar ruwa mai nisa a cikin tashar tashar jiragen ruwa a kusa da tashar jiragen ruwa. An yi amfani da diamita na hydraulic 4 tsakanin allo na ƙarshe da sanda, kuma tsayin fitarwa shine diamita na hydraulic 11.
Tsarin tsari na bututu Venturi da aka yi amfani da shi don auna saurin shigar shigar (tsawon millimeters).An ƙirƙira tare da Openscad 2021.01, openscad.org.
Kula da matsa lamba a kan ɗayan fuskoki na sandar tsakiya ta hanyar matsi na 0.5 mm a tsakiyar jirgin sama na sashin gwaji. Diamita na famfo ya dace da 5 ° angular tazara;saboda haka daidaitattun angular yana da kusan 2 °. Ana iya juya sandar da aka kula da ita game da axis, kamar yadda aka nuna a cikin Hoto 3. Bambanci tsakanin ma'aunin igiya da matsa lamba a ƙofar sashin gwajin ana auna shi tare da nau'in DP Cell Honeywell SCX.
Ana nuna ganuwar tashoshi a cikin launin toka. Ruwa yana gudana daga hagu zuwa dama kuma sanda ya toshe shi. Lura cewa ra'ayi "A" yana daidai da igiya.
Makasudin gwajin shine don aunawa da fassara fassarar matsa lamba tsakanin tashar tashar tashar da matsa lamba a saman sandar cibiyar, \ (\theta \) da \ (\ alpha \) don azimuths da dips daban-daban. Don taƙaita sakamakon, za a bayyana matsa lamba a cikin nau'i marar girma kamar lambar Euler:
inda \(\rho \) shine yawan ruwa, \({u}_{i}\) shine madaidaicin saurin shiga, \({p}_{i}\) shine matsa lamba, kuma \({p }_{ w}\) shine matsa lamba a wani wuri da aka ba akan bangon sandar. An saita saurin shigarwar a cikin kewayo daban-daban guda uku da aka ƙaddara a cikin kewayon madaidaicin madaidaicin m 6. zuwa tashar Reynolds lambar, \(Re\equiv {u}_{i}H/\nu \) (inda \(H\) shine tsayin tashar, kuma \(\nu \) shine dankowar kinematic) tsakanin 40,000 da 67,000. The sanda Reynolds number (\(Re\equiv}0) daga 0 zuwa 5 (\(Re\equiv})) Ƙarfin tashin hankali da aka kiyasta ta daidaitattun daidaitattun sigina na sigina da aka rubuta a cikin venturi shine 5% akan matsakaita.
Hoto na 4 yana nuna alaƙar \ ({Eu}_{w} \) tare da kusurwar azimuth \ (\ theta \), wanda aka kwatanta da kusurwoyi uku na dip, \ (\ alpha \) = 30 °, 50 ° da 70 ° . Ana rarraba ma'auni a cikin jadawalai uku bisa ga diamita na sandar. Ana iya ganin cewa ba za a iya gani ba a cikin lambobi masu zaman kansu. θ yana biye da yanayin da aka saba da shi na bangon bango a kusa da kewayen shingen madauwari. A magudanar da ke gudana, watau, θ daga 0 zuwa 90 °, matsa lamba bangon sanda yana raguwa, ya kai mafi ƙanƙanta a 90 °, wanda ya dace da rata tsakanin sandunan inda saurin ya fi girma saboda iyakokin yanki na kwarara. Bayan haka, 0 daga matsa lamba zuwa 0 ° bayan 0 daga matsa lamba zuwa 0. uniform saboda rabuwa na baya iyaka Layer na sandar bango. Lura cewa babu wani canji a cikin kwana na m matsa lamba, wanda ya nuna cewa yiwuwar tashin hankali daga kusa karfi yadudduka, kamar Coanda effects, su ne na biyu.
Bambance-bambancen lambar Euler na bangon da ke kewaye da sanda don kusurwoyi daban-daban na karkata da diamita na sanda. An yi shi tare da Gnuplot 5.4, www.gnuplot.info.
A cikin wadannan, muna nazarin sakamakon bisa zaton cewa Euler lambobin za a iya kiyasta kawai ta hanyar geometric sigogi, watau siffa tsawon rabo \ (d/g \) da \ (d / H \) (inda \ (H \) ne tashar ta tsawo) da kuma karkata \ (\ alpha \) .A rare m ka'ida na babban yatsa ya bayyana cewa ruwa tsarin da aka ƙaddara a kan yadi tsarin aiki a kan yadi tsarin da karfi a kan yatsan sanda. axis, \({u}_{n}={u}_{i}\mathrm {sin} \alpha \) .Wani lokaci ana kiran wannan ka'idar 'yancin kai. Daya daga cikin manufofin bincike na gaba shine bincika ko wannan ka'ida ta shafi shari'ar mu, inda kwarara da toshewa ke tsare a cikin rufaffiyar tashoshi.
Bari mu yi la'akari da matsa lamba da aka auna a gaban tsaka-tsakin sandar matsakaici, watau θ = 0. Bisa ga ma'auni na Bernoulli, matsa lamba a wannan matsayi \ ({p}_{o} \) ya gamsu:
inda \ ({u}_{o} \) shine saurin ruwa kusa da bangon sanda a θ = 0, kuma muna ɗaukar ƙananan asarar da ba za a iya jurewa ba. Lura cewa matsa lamba mai ƙarfi yana da zaman kanta a cikin lokacin makamashin motsi. Idan \ ({u}_{o} \) ya zama fanko (watau yanayin tsautsayi), Euler \ lambobi ya kamata a haɗa kai. Duk da haka, za a iya lura da sakamakon \ (E 0) _{w}\) yana kusa da amma ba daidai yake daidai da wannan darajar ba, musamman ga manyan kusurwoyi masu girma. Wannan yana nuna cewa saurin da ke kan sandar sanda ba ya ɓacewa a \ (\ theta = 0 \), wanda za'a iya kashe shi ta hanyar ƙaddamar da layi na yanzu da aka yi ta hanyar sandar karkatar. Tun da ya kwarara yana iyakance zuwa sama da kasa na gwajin gwaji ya kamata ya haifar da raguwa a cikin sassan da ke ƙasa, wannan ya kamata ya haifar da raguwar raguwa a cikin sashin gwaji. rera gudu a saman. Idan aka ɗauka cewa girman jujjuyawar da ke sama ita ce tsinkayar saurin shigar da ke kan shaft (watau \ ({u}_{i}\mathrm{cos}\alpha \)), sakamakon lambar Euler daidai shine:
Hoto na 5 yana kwatanta daidaito. p}_{e} \), Har ila yau yana bin yanayin da ya dace da \({\mathrm{sin}}^{2}\alpha \) .A cikin duka biyun, duk da haka, ƙididdiga ya dogara ne akan diamita na sanda, wanda yake da kyau tun lokacin da karshen ya ƙayyade wurin da aka hana. Wannan fasalin yana kama da raguwar matsa lamba na wani farantin karfe, inda aka rage magudanar tashoshi ta wani bangare a cikin takamaiman wuraren gwajin. wannan yanayin, matsa lamba ya sauko sosai a cikin maƙarƙashiya kuma wani ɓangare yana murmurewa yayin da yake faɗaɗa baya. Yin la'akari da ƙuntatawa azaman toshewa daidai gwargwado ga axis na sanda, ana iya rubuta matsi tsakanin gaba da baya na sandar kamar 18:
inda \({c}_{d}\) shine madaidaicin ja da ke bayyana sashin dawo da matsa lamba tsakanin θ = 90° da θ = 180°, da kuma \({A}_{m}\) da \ ({A}_{f}\) shine mafi ƙarancin ɓangaren giciye kyauta a kowane tsawon raka'a daidai gwargwado ga ma'aunin sandar, kuma dangantakarsa da diamita \{} (g+d\ dama)/g\)) Lambobin Euler masu dacewa sune:
Lambar Euler ta bango a \ (\theta = 0 \) azaman aikin dip. Wannan madaidaicin yayi dace da ma'auni.(3).An ƙirƙira tare da Gnuplot 5.4, www.gnuplot.info.
Lamba Euler na bango yana canzawa, a cikin \(\theta =18{0}^{o}\) (cikakkiyar alamar) da kuma fita (alamar wofi) tare da tsoma baki. Waɗannan lambobi sun dace da ka'idar 'yancin kai, watau \ (Eu\propto {\mathrm{sin}}}^{2}\alpha \) . An ƙirƙira tare da Gnuplot 5.4, a cikin www.gnup.gnup.
Hoto na 7 yana nuna dogara ga \({Eu}_{0-180}/{\mathrm{sin}}}^{2}\alpha \) akan \(d/g\), yana nuna matsananciyar Kyakkyawan daidaito. bari sashin gwajin ya bi irin wannan yanayin, amma tare da ƙididdiga daban-daban waɗanda ke yin la'akari da dawo da matsa lamba a cikin sarari na baya tsakanin mashaya da tashar tashar tashar tashar.
Matsakaicin ja yana da alaƙa da matsa lamba na gaba da bayan sanda \ (\ hagu ({Eu}_{0-180} \ dama) \) da jimlar matsa lamba tsakanin tashar tashar tashar da fitarwa. Yankin launin toka shine 67% amintaccen band don daidaitawa. An ƙirƙira tare da Gnuplot 5.gnuplot.
Mafi qarancin matsin lamba \ ({P} \ _ gparnan da ke tsakanin sanduna na yanzu, da gudu a tsakiyar abin da ke tsakanin sanduna ({g Kuliji tare da midpoint na tashar) yana da alaƙa da waɗannan abubuwan:
Matsalolin \ ({p}_{g} \) na iya zama alaƙa da matsi na sandar a θ = 90 ° ta hanyar haɗawa da rarraba matsa lamba akan rata da ke raba sandar tsakiya tsakanin tsakiyar tsakiya da bango (duba Hoto 8).Ma'aunin iko yana bada 19:
inda \ (y \) shine daidaitawa na al'ada zuwa saman sanda daga tsakiya na rata tsakanin sandunan tsakiya, kuma \ (K \) shine curvature na layin yanzu a matsayi \ (y \) . Don kimantawa na nazarin matsa lamba akan saman sanda, muna ɗauka cewa \ ({u}_{g} \) daidai ne kuma \ (K \ hagu \) an ƙididdige shi ta hanyar ƙididdigewa. A jikin bangon sanda, ana ƙaddara curvature ta ɓangaren ellipse na sanda a kusurwar \ (\ alpha \), watau \ (K \ hagu(g/2 \ dama) = \ hagu (2/d \ dama) {\ mathrm{sin} }^{2}\alpha \) (duba Hoto 8).Sa'an nan, game da curvature of the streamline \ streamline coordinated streamline. ordinate \(y \) yana bayarwa ta:
Fasalin kallon giciye, gaba (hagu) da sama (kasa).An ƙirƙira da Microsoft Word 2019,
A gefe guda, ta hanyar kiyaye yawan jama'a, matsakaicin saurin gudu a cikin jirgin sama daidai gwargwado a wurin aunawa \(\langle {u}_{g}\rangle \) yana da alaƙa da saurin shigar:
inda \({A}_{i}\) shine yankin magudanar ruwa a mashigar tashar kuma \({A}_{g}\) shine yankin ma'aunin ma'auni (duba siffa 8) bi da bi ta :
Lura cewa \({u}_{g}\) baya daidaita da \(\langle {u}_{g}\rangle \) .Hakaka, Hoto na 9 yana nuna ma'aunin gudun \({u}_{g}/\langle {u}_{g}\rangle \), wanda aka ƙididdige shi ta hanyar ƙididdiga.(10)–(14), wanda aka ƙirƙira bisa ga yanayin da ake iya ganowa. wanda aka yi ta hanyar oda na biyu:
Matsakaicin matsakaicin\({u}_{g}\) da matsakaita\(\langle {u}_{g}\rangle \) saurin tashar cibiyar giciye-sashe \(.\) Ƙaƙƙarfan madaidaicin madaidaicin ma'auni.
Hoto na 10 ya kwatanta \({Eu}_{90}\) tare da sakamakon gwaji na lissafin.(16) Matsakaicin karkacewar dangi shine 25%, kuma matakin amincewa shine 95%.
Lambar bangon Euler a \(\theta ={90}^{o}\) .Wannan lanƙwan yayi daidai da ma'auni.(16).An ƙirƙira da Gnuplot 5.4, www.gnuplot.info.
Za'a iya ƙididdige ƙarfin net ɗin \({f}_{n}\) da ke aiki akan sandar tsakiya daidai gwargwado ga axis ɗin ta ta hanyar haɗa matsi akan saman sandar kamar haka:
inda madaidaicin farko shine tsayin sanda a cikin tashar, kuma ana yin haɗin kai tsakanin 0 da 2π.
Hasashen \({f}_{n}\) a kan hanyar ruwan ya kamata ya dace da matsa lamba tsakanin mashigai da mashigar tasha, sai dai idan jujjuyawar ta yi daidai da sanda da ƙarami saboda rashin ci gaban sashin gaba.Don haka,
Hoto na 11 yana nuna hoto na ma'auni.(20) ya nuna kyakkyawar yarjejeniya ga duk yanayin gwaji. Duk da haka, akwai ƙananan 8% ƙetare a hannun dama, wanda za'a iya danganta shi da amfani da shi azaman ƙididdiga na rashin daidaituwa tsakanin tashar tashar tashar tashar tashar tashar tashar da fitarwa.
Ma'aunin wutar lantarki na tashar.Layin ya dace da ma'auni.(20) .Ƙararren haɗin gwiwar Pearson ya kasance 0.97. An halicce shi tare da Gnuplot 5.4, www.gnuplot.info.
Canza madaidaicin kusurwar sandar, matsa lamba a bangon sandar sanda da raguwar matsa lamba a cikin tashar tare da layin madaidaiciya na sandunan cylindrical huɗu masu karkata an auna su.An gwada manyan igiyoyi daban-daban guda uku. matsakaicin a gaba kuma mafi ƙanƙanta a rata ta gefe tsakanin sanduna, murmurewa a ɓangaren baya saboda rabuwar iyaka.
Ana nazarin bayanan gwaji ta amfani da la'akari da kiyayewa na lokaci-lokaci da ƙididdigar ƙima don nemo lambobi marasa daidaituwa waɗanda ke da alaƙa da lambobin Euler zuwa ma'auni na tashoshi da sanduna.Dukan siffofi na geometric na toshe suna da cikakkiyar wakilci ta hanyar rabo tsakanin diamita na sanda da rata tsakanin sanduna (a gefe) da tsayin tashar (a tsaye).
An samo ƙa'idar 'yancin kai don yawancin lambobin Euler waɗanda ke nuna matsi a wurare daban-daban, watau idan matsa lamba ba ta da girma ta amfani da tsinkayar saurin shigar da ke daidai da sanda, saitin ya kasance mai zaman kansa daga kusurwar tsomawa.Bugu da ƙari, fasalin yana da alaƙa da taro da haɓakar kwararan matakan kiyayewa sun daidaita kuma suna goyan bayan ƙa'idodin ƙa'idar da ke sama.Sai kawai matsa lamba a saman sanda a rata tsakanin sanduna ya bambanta kaɗan daga wannan ka'ida. An haifar da haɓakar haɓakar haɓakar haɓakar haɓaka waɗanda za a iya amfani da su don tsara irin na'urorin hydraulic irin wannan. 1,22,23,24.
Wani sakamako mai ban sha'awa na musamman ya fito ne daga nazarin raguwar matsa lamba tsakanin mashigai da fitarwa na sashin gwaji. A cikin rashin tabbas na gwaji, sakamakon ja da ƙima yana daidai da haɗin kai, wanda ke nuna kasancewar waɗannan sigogi masu zuwa:
Yi la'akari da girman \ (\ hagu (d/g+2 \ dama) d/g \) a cikin ma'auni na ma'auni.(23) shine girman girman baka a cikin ma'auni.(4), in ba haka ba ana iya ƙididdige shi tare da mafi ƙanƙanta da sashin giciye na kyauta daidai da sanda, \ ({A}_{m}\) da ({A}_{m}\) da kuma \({A}_{m}\) da kuma \({A} Wannan shine a cikin kewayon Rey zuwa ga tsohon lambobi). binciken na yanzu (40,000-67,000 don tashoshi da 2500-6500 don sanduna) . Yana da mahimmanci a lura cewa idan akwai bambancin zafin jiki a cikin tashar, zai iya rinjayar yawan ruwa.
Ruck, S., Köhler, S., Schlindwein, G., da Arbeiter, F. Canja wurin zafi da ma'auni na matsa lamba a cikin tashar da aka yi ta hanyar haƙarƙari daban-daban akan bango. gwani. Canja wurin zafi 31, 334-354 (2017).
Wu, L., Arenas, L., Graves, J., da Walsh, F. Fassarar tantanin halitta: hangen nesa mai gudana, raguwar matsa lamba, da jigilar jama'a a cikin na'urori masu girma biyu a cikin tashoshi rectangular.J.Electrochemistry.Jam'iyyar Socialist.167, 043505 (2020).
Liu, S., Dou, X., Zeng, Q. & Liu, J. Mahimman sigogi na tasirin Jamin a cikin capillaries tare da ƙunshewar sassan giciye.J.Man fetur.kimiyya.Birtaniya.196, 107635 (2021).