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<!DOCTYPE ArticleSet PUBLIC "-//NLM//DTD PubMed 2.7//EN" "https://dtd.nlm.nih.gov/ncbi/pubmed/in/PubMed.dtd">
<ArticleSet>
<Article>
<Journal>
				<PublisherName>انجمن هیدرولیک ایران</PublisherName>
				<JournalTitle>نشریه علمی هیدرولیک</JournalTitle>
				<Issn>2345-4237</Issn>
				<Volume>6</Volume>
				<Issue>4</Issue>
				<PubDate PubStatus="epublish">
					<Year>2012</Year>
					<Month>01</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Investigation of Effective Parameters on the Hydrofoil Performance near the Free Surface of Water</ArticleTitle>
<VernacularTitle>بررسی پارامترهای موثر بر عملکرد هیدروفویل در نزدیکی سطح آب</VernacularTitle>
			<FirstPage>1</FirstPage>
			<LastPage>17</LastPage>
			<ELocationID EIdType="pii">85405</ELocationID>
			
<ELocationID EIdType="doi">10.30482/jhyd.2012.85405</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>محمدحسن</FirstName>
					<LastName>جوارشکیان</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>علی</FirstName>
					<LastName>اسماعیلی</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2011</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</History>
		<Abstract>In this study, a numerical method is used to assess the effect of thickness, camber, submergence depth&lt;br /&gt;and flow velocity around a submerged hydrofoil. A pressure based algorithm is used to solve Navierstokes&lt;br /&gt;equations, and Volume of Fluid (VOF) approach is applied to simulate two-phase fluid (water&lt;br /&gt;and air). The model and second order upwind scheme have been used for turbulence models and&lt;br /&gt;differential schemes, respectively. For verifying, a part of results is compared with published&lt;br /&gt;experimental results. The numerical and experimental results show excellent agreement; thus, the&lt;br /&gt;process of numerical simulations is confirmed. The results of this study illustrate that the lift and drag&lt;br /&gt;coefficients increase with rising the thickness of the hydrofoil, but the lift to drag ratio has a&lt;br /&gt;downward trend. On the other hand, the lift and drag coefficients increase with growing the camber of&lt;br /&gt;the hydrofoil, but lift to drag ratio has upward trend. Therefore, to opt the best section of the hydrofoil,&lt;br /&gt;the less thickness and the high camber are more desirable to getting high hydrodynamic performance.&lt;br /&gt;The switched of the hydrofoil section obviously affects the airflow and boundary layer formed on the&lt;br /&gt;free surface of water. Moreover, lift and drag coefficients become high by increasing the submergence&lt;br /&gt;depth and angle of attack, as a result lift to drag ratio increases. Lift and drag coefficients are&lt;br /&gt;decreased by increasing flow velocity, and lift to drag ratio has a downward trend.</Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
<ArchiveCopySource DocType="pdf">https://jhyd.iha.ir/article_85405_af0a19cbbf7ec9e02e05bfa2e227ba21.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>انجمن هیدرولیک ایران</PublisherName>
				<JournalTitle>نشریه علمی هیدرولیک</JournalTitle>
				<Issn>2345-4237</Issn>
				<Volume>6</Volume>
				<Issue>4</Issue>
				<PubDate PubStatus="epublish">
					<Year>2012</Year>
					<Month>01</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Coupled Analysis of Fluid Transients and Structural Dynamic Responses in Pipelines by MOC-FDM</ArticleTitle>
<VernacularTitle>تحلیل همزمان جریان غیرماندگار و پاسخ های دینامیکی سازه خطوط لوله به روش MOC-FDM</VernacularTitle>
			<FirstPage>19</FirstPage>
			<LastPage>31</LastPage>
			<ELocationID EIdType="pii">85406</ELocationID>
			
<ELocationID EIdType="doi">10.30482/jhyd.2012.85406</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>سید محمود</FirstName>
					<LastName>جزایری مقدس</LastName>
<Affiliation>دانشگاه شهید چمران</Affiliation>

</Author>
<Author>
					<FirstName>حسین</FirstName>
					<LastName>محمدولی سامانی</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2011</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</History>
		<Abstract>Water hammer is a type of transient flow in pipelines which may in general be produced due to valve&lt;br /&gt;closure or sudden shut down of pumps. Transient flow creates sudden variation in the velocity and&lt;br /&gt;pressure of fluid flow in the pipelines which in effect may induce some dynamic vibrations in the&lt;br /&gt;structure of pipe. Furthermore, such structural vibrations can affect the fluid flow. Taking into account&lt;br /&gt;them is necessary for modeling of fluid-structure interaction. In this paper the fluid-structural&lt;br /&gt;interaction (FSI) of water hammer in pipeline systems are investigated. Two sets of hydraulic and&lt;br /&gt;structural equations with common variables have been numerically analyzed through MOC-FDM&lt;br /&gt;simultaneous solving process which has been prepared by a computer-assisted program. Some&lt;br /&gt;examples have been solved by this method, with satisfactory results. This indicates that fluid-structure&lt;br /&gt;interaction can have critical effect on the value of fluid pressure.</Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
<ArchiveCopySource DocType="pdf">https://jhyd.iha.ir/article_85406_a9f9a8a150d14a59a3cdaa03337a1360.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>انجمن هیدرولیک ایران</PublisherName>
				<JournalTitle>نشریه علمی هیدرولیک</JournalTitle>
				<Issn>2345-4237</Issn>
				<Volume>6</Volume>
				<Issue>4</Issue>
				<PubDate PubStatus="epublish">
					<Year>2012</Year>
					<Month>01</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>The Effect of Wastewater on the Non-Settling Velocity and Shear Stress of Cohesive Sediments</ArticleTitle>
<VernacularTitle>تاثیر پساب شهری بر سرعت و تنش برشی غیررسوبگذار رسوبهای چسبنده</VernacularTitle>
			<FirstPage>33</FirstPage>
			<LastPage>42</LastPage>
			<ELocationID EIdType="pii">85407</ELocationID>
			
<ELocationID EIdType="doi">10.30482/jhyd.2012.85407</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>میلاد</FirstName>
					<LastName>خواستار بروجنی</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>حسین</FirstName>
					<LastName>صمدی بروجنی</LastName>
<Affiliation>عضو هیات علمی دانشگاه شهرکرد</Affiliation>

</Author>
<Author>
					<FirstName>کاظم</FirstName>
					<LastName>اسماعیلی</LastName>
<Affiliation></Affiliation>
<Identifier Source="ORCID">0000-0001-5354-0949</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2011</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</History>
		<Abstract>Sedimentation in open channels is one of the basic problems in the management of irrigation&lt;br /&gt;networks. Complexity of behavior of cohesive sediment transport makes determination of the criteria&lt;br /&gt;for open channel design to be difficult. The purpose of this study is to determine non-settling velocity&lt;br /&gt;and non-settling shear stress for open channel flow containing wastewater and suspended cohesive&lt;br /&gt;sediment. Experiments were carried out in an annular flume located in the hydraulic laboratory of&lt;br /&gt;Shahrekord University, Iran. The sediment samples were taken from Pirbalut dam reservoir, located&lt;br /&gt;upstream of Northern Karun basin. The result showed that wastewater content in flow causes the&lt;br /&gt;suspended sediment deposition and flocculation to be likely increased. It also caused the threshold of&lt;br /&gt;non-settling velocity to be increased at a rate of 10% compared to pure water. A similar result was also&lt;br /&gt;obtained for threshold of shear stress. The results obtained from this study were compared and the&lt;br /&gt;results showed that the empirical methods were not capable in calculating non-settling velocity for&lt;br /&gt;open channel flow containing waste water and suspended cohesive sediments. The results also showed&lt;br /&gt;that the Froud number should be more than 0.47 for non-settling condition of suspended cohesive&lt;br /&gt;sediments.</Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
<ArchiveCopySource DocType="pdf">https://jhyd.iha.ir/article_85407_62e5bd018861ec37550bc5239a60133a.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>انجمن هیدرولیک ایران</PublisherName>
				<JournalTitle>نشریه علمی هیدرولیک</JournalTitle>
				<Issn>2345-4237</Issn>
				<Volume>6</Volume>
				<Issue>4</Issue>
				<PubDate PubStatus="epublish">
					<Year>2012</Year>
					<Month>01</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Development of a Numerical Model for Predicting Dynamic Pressures in Open Channel Flow using Non-Orthogonal Curvilinear Coordinate Grid</ArticleTitle>
<VernacularTitle>توسعه مدل عددی برای پیش بینی فشارهای دینامیک در جریان کانال های باز با شبکه منحنی الخط غیرمتعامد</VernacularTitle>
			<FirstPage>43</FirstPage>
			<LastPage>58</LastPage>
			<ELocationID EIdType="pii">85408</ELocationID>
			
<ELocationID EIdType="doi">10.30482/jhyd.2012.85408</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>زهره</FirstName>
					<LastName>دهقان بهابادی</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>محمدرضا</FirstName>
					<LastName>هادیان</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>امیررضا</FirstName>
					<LastName>زراتی</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2011</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</History>
		<Abstract>A 2DV numerical model is developed for solving unsteady Navier-Stokes equations with the ability&lt;br /&gt;for calculating dynamic pressures in non-orthogonal curvilinear coordinate grids for free surface&lt;br /&gt;flows. The model is based on fractional step method (or projection method). The free surface elevation&lt;br /&gt;is calculated using continuity equation. The present method uses the advantages of shallow water&lt;br /&gt;models for calculating free surface elevation (even in cases with large changes) and benefits the&lt;br /&gt;flexibility of moving non-orthogonal grids. Moreover, this method presents the ability of developing a&lt;br /&gt;shallow water solver to take into account the dynamic pressures.&lt;br /&gt;The simulation of water elevation in a gradually varied flow, showed the ability of mesh adaption in&lt;br /&gt;moving and curved boundaries. Comparing the results of the model with experimental data and other&lt;br /&gt;numerical models, for flow passing over a hump and trench, confirms the ability of the developed&lt;br /&gt;model for simulating the free surface flows. Having the ability of calculating free surface and dynamic&lt;br /&gt;pressures, the model can therefore be applied to rapidly varied flows.</Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
<ArchiveCopySource DocType="pdf">https://jhyd.iha.ir/article_85408_8e1853b6a873a42959e1b8a70e9dc702.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>انجمن هیدرولیک ایران</PublisherName>
				<JournalTitle>نشریه علمی هیدرولیک</JournalTitle>
				<Issn>2345-4237</Issn>
				<Volume>6</Volume>
				<Issue>4</Issue>
				<PubDate PubStatus="epublish">
					<Year>2012</Year>
					<Month>01</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Armoring Effect on Local Scouring around the Bridge Pier under (Part1 :) Steady Flow</ArticleTitle>
<VernacularTitle>مطالعه تاثیر لایه سپری بر آب شستگی پایه پل، تحت اثر جریان دائمی (بخش یکم)</VernacularTitle>
			<FirstPage>59</FirstPage>
			<LastPage>75</LastPage>
			<ELocationID EIdType="pii">85409</ELocationID>
			
<ELocationID EIdType="doi">10.30482/jhyd.2012.85409</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>عبدالرضا</FirstName>
					<LastName>کبیری سامانی</LastName>
<Affiliation>دانشیار، دانشکده مهندسی عمران، دانشگاه صنعتی اصفهان</Affiliation>
<Identifier Source="ORCID">0000-0002-5984-3892</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2011</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</History>
		<Abstract>In this study armoring effect on local scouring around bridge pier under steady flow condition was&lt;br /&gt;investigated based on model experimentation. Different combinations of bed-armor layers were&lt;br /&gt;employed. Three circular piers of 22, 33 and 42 mm were used. Results show that while small bed&lt;br /&gt;particles are under the protective effect of armor layer, increasing the total scouring depth, yields an&lt;br /&gt;increase in the secondary armor layer depth until the armor layer itself is not influenced by the horseshoe&lt;br /&gt;vortices. The minimum stabilized secondary armor layer is identical to the armor grain size.&lt;br /&gt;Results showed that there is not meaningful correlation between total scouring depth and B/d (where B&lt;br /&gt;is the pier diameter and d is the mean bed grain sizes) for B=33 and 42 mm. However for B=22 mm,&lt;br /&gt;increasing B/d tends to increase the total scouring depth. For the armor layer particles size of 2.36 mm&lt;br /&gt;the armoring effect for B=22 mm is vanished. The most important parameters in evolution of scouring&lt;br /&gt;depth are the armor layer grain size and the armor layer thickness.</Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
<ArchiveCopySource DocType="pdf">https://jhyd.iha.ir/article_85409_f0f915de822b7ed9230c5c4a7998210b.pdf</ArchiveCopySource>
</Article>

<Article>
<Journal>
				<PublisherName>انجمن هیدرولیک ایران</PublisherName>
				<JournalTitle>نشریه علمی هیدرولیک</JournalTitle>
				<Issn>2345-4237</Issn>
				<Volume>6</Volume>
				<Issue>4</Issue>
				<PubDate PubStatus="epublish">
					<Year>2012</Year>
					<Month>01</Month>
					<Day>21</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Study of Dynamic Pressure Distribution over the Bed of Compound Flip Buckets</ArticleTitle>
<VernacularTitle>مطالعه توزیع فشار دینامیکی بر روی بستر پرتاب کننده جامی مرکب</VernacularTitle>
			<FirstPage>77</FirstPage>
			<LastPage>90</LastPage>
			<ELocationID EIdType="pii">85410</ELocationID>
			
<ELocationID EIdType="doi">10.30482/jhyd.2012.85410</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>امید</FirstName>
					<LastName>امین الرعایایی یمینی</LastName>
<Affiliation></Affiliation>

</Author>
<Author>
					<FirstName>محمدرضا</FirstName>
					<LastName>کاویانپور</LastName>
<Affiliation></Affiliation>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2011</Year>
					<Month>03</Month>
					<Day>21</Day>
				</PubDate>
			</History>
		<Abstract>Flip buckets are usually placed at the end of chute spillways or outlet conduits of high dams. The&lt;br /&gt;projected jets from these buckets jump into plunge pools to dissipate the destructive energy of&lt;br /&gt;plunging jets. Compound flip bucket is a special bucket with a non-zero degree of cross sectional&lt;br /&gt;slope, followed by a curvature in its longitudinal direction. These structures are very suitable for&lt;br /&gt;restricted geometries and conditional topographies. Although, studies of flow over flip buckets started&lt;br /&gt;many years ago and valuable information is available for similar buckets, still there are uncertainties&lt;br /&gt;regarding the flow over compound flip buckets. Therefore, in this study the hydraulic parameters such&lt;br /&gt;as pressure, velocity and depth of flow on these structures were evaluated. Two chute spillways with&lt;br /&gt;their flip buckets were used to check the pressure distribution and its variation with different hydraulic&lt;br /&gt;characteristic along the compound flip buckets. The scaled model of Gotvand dam (south of Iran) at&lt;br /&gt;Water Research Institute of Iran was used for this study. The Froude number varies in the range of 3.5&lt;br /&gt;to 7.5. The results are presented in the form of dimensionless equations, which are calibrated based on&lt;br /&gt;the present results. The location of maximum dynamic pressure on the bed of the compound flip&lt;br /&gt;bucket is also determined.</Abstract>
			<OtherAbstract Language="FA"></OtherAbstract>
<ArchiveCopySource DocType="pdf">https://jhyd.iha.ir/article_85410_0f26f3dbc43ed58b11ca7e90f40acea7.pdf</ArchiveCopySource>
</Article>
</ArticleSet>
