黏性流体的一维定常流动-习题答案.docx

上传人(卖家):最好的沉淀 文档编号:6255999 上传时间:2023-06-19 格式:DOCX 页数:7 大小:64.93KB
下载 相关 举报
黏性流体的一维定常流动-习题答案.docx_第1页
第1页 / 共7页
黏性流体的一维定常流动-习题答案.docx_第2页
第2页 / 共7页
黏性流体的一维定常流动-习题答案.docx_第3页
第3页 / 共7页
黏性流体的一维定常流动-习题答案.docx_第4页
第4页 / 共7页
黏性流体的一维定常流动-习题答案.docx_第5页
第5页 / 共7页
点击查看更多>>
资源描述

1、【例题解析】第六章 黏性流体的一维定常流动V例 6-1管道直径 d = 100mm , 输送水的流量 q = 0.01 m3/s ,水的运动黏度 n = 110 -6 m2/s, 求水在管中的流动状态?若输送n = 1.14 10 -4 m2/s的石油, 保持前一种情况下的流速不变,流动又是什么状态?解:(1)雷诺数Re = VdnV = 4qVpd 2= 4 0.013.14 0.12= 1.27 ( m/s)故水在管道中是紊流状态。Re = 1.27 0.1 = 1.27 105 2000110 -6(2)Re = Vd =n1.27 0.11.14 10 -4= 1114 2000故油在

2、管中是层流状态。例 6-2有一长方形风道长 l = 40m, 截面积 A = 0.50.8m2 ,管壁绝对粗糙度 = 0.19mm,输送t = 20的空气,流量 qV解:平均流速= 21600m3/h,试求在此段风道中的沿程损失。当量直径V = qVA=21600= 15 (m/s)3600 0.5 0.8de =2hb h + b= 2 0.5 0.8 = 0.615 (m)0.5 + 0.820空气的运动黏度n = 1.6310-5m2/s,密度= 1.2kg/m3。雷诺数Re = Vden= 15 0.615 = 565950 1.6310 -5相对粗糙度查莫迪曲线图得l = 0.016

3、5 = 0.19 = 0.00031d e615沿程损失Vl2hf = l= 0.016540 152= 12.3 (m 空气柱)de 2g0.6152 9.806沿程压强损失pf = hf rg = 12.3 9.806 1.2 = 144.8 (Pa)例 6-3 如图 6-1 所示,水平短管从水深 H = 16m 的水箱中排水至大气中,管路直径d1 = 50mm, d 2 = 70mm,阀门阻力系数z 门 = 4.0,只计局部损失,不计沿程损失,并认为水箱容积足够大,试求通过此水平短管的流量。解: 列截面 00 和 11 的伯努利方程V 2H + 0 + 0 = 0 + 0 + 1 +(z

4、+ z+ zV 2+ z ) 12g入由表查得z 入=0.5, z 扩1 =0.24, z 缩2 =0.30,故扩1缩2门 2g12gH1+ z 入 + z 扩1 + z 缩2 + z 门V1 =11+ 0.5 + 0.24 + 0.30 + 4.02 9.806 16= 7.2 (m/s)通过水平短管的流量q = V p d 2 = 7.2 p 0.052 = 0.01413 (m3/s)V1 4 14图 6-1 例 6-3 示意图图 6-2 例 6-4 示意图311例 6-4有一并联管道如图 6-2 所示。若已知 qV = 300m /h, d = 100mm, l = 40m,d 2 =

5、 50mm,l2 = 30m,d 3 = 150mm,l3 = 50m,l1 = l2 = l3 = 0.03。试求各支管中的流量 qV 1 、qV 2 、 qV 3 及并联管道中的水头损失。解:根据并联管道的流动规律因此有qV = qV 1 + qV 2 + qV 3hf1 = hf2 = hf3l V 2l V 2l V 2(a)111l 11 = l 22 = l 33 d1 2gd 2 2gd 3 2g401 4q20.030.1 V 1 2 9.806 p 0.12 3014q 2= 0.030.05 V 22 9.806 p 0.052 5014q 2= 0.030.15 V 32

6、 9.806 p 0.152 9898.98qV 1 = 238873.79qV 2 = 1634.8qV 3所以qV 2 = 0.2qV1 (b)将式(b)代入式(a)中qV 3= 2.46qV 1 qV = qV 1 + 0.2qV 1 + 2.46qV 1qV = 3.66qV 1所以qV 1= qV3.66= 300 = 81.97 (m3/h)3.66V 2V 1q= 0.2q= 0.2 81.97 = 16.36 (m3/h)V 3V 1q= 2.46q= 2.46 81.97 = 201.65 (m3/h)并联管道的水头损失l V 24014 81.97 2hf(a-b) = h

7、f1 = l1 11 = 0.03 = 5.15 (mH2O)d1 2g0.12 9.806 3600p 0.12 SVa例 6-5如图 6-3 所示,虹吸管总长l =21m,坝顶中心前管长l =8m。管内径 d =0.25m, 坝顶中心与上游水面的高度差 h1 =3.5m,二水位落差 h2 =4m。设沿程阻力系数l =0.03,虹吸管进口局部阻力系数V 1 =0.8,出口局部阻力系数V 2 =1,三个 45折管的局部阻力系数均为0.3,试求虹吸管的吸水流量 q 。若当地的大气压强 p =105Pa,水温t =20,所对应的水的密度=998kg/m3,水的饱和压强 p =2.42103Pa,试

8、求最大吸水高度。图 6-3 例 6-5 示意图解:对上下游液面列伯努利方程,得pa = -pa l V 2所以流速V =rgh2 + rg + l d +2gh2l l + Vd2 9.8 40.03 21 + (0.8 +1+ 0.3 3)0.25=V 2g= 3.875 m/sp2qV = 0.25 4 3.875 = 0.19 m3/s对上游液面和坝顶中心列伯努利方程,得pa =p2V 2 l V 2rgh1 + rg + 2g + l d+ V 1 2g+ V 1 2g = 1 +1+ l l + Vpa - p2rg= h + 1+ l l1 d V 2hd1 h2l l +Vd当

9、p2 = p S ,可得最大吸水高度h1 pa - pSrg1+ l l + V1- dlh2 =(100 - 2.42) 103 -998 9.81+ 0.032180.25+ (0.8 + 0.3) 4 = 7.63 ml d + V0.03+ (0.8 +1+ 0.3 3)0.25可见最大吸水高度为 7.63m,现吸水高度为 3.5m,远小于最大吸水高度,所以不会出现水的汽化,故虹吸作用不会被破坏。一般而言,虹吸管的吸水高度不得超过 7m。例 6-6 某厂有一条铸铁输水管线,如图 6-4 所示,长 500m,直径 200mm,流量为 100L/s,水源为 5m深井;进口有一滤网( =5.

10、2),管路中有 10 个 90弯头( =0.48),两个闸门( =0.08),运动黏度系数n =1.3mm2/s,绝对粗糙度 =1.3mm,2 截面与水泵轴线在同一水平面上。求水泵所需压头。解:在 1 和 2 截面间建立能量方程V 2H = 5 + 2g + hWV = 4qVpd 2= 4 100 10-33.14 0.22= 3.18 m/s由Re = Vd = 4.9 105 , = 0.0065 ,可由莫迪图查得沿程nd损失系数l = 0.033 ,则图 6-4 例 6-6 示意图l V 2500 3.182hW = V + l d = 5.2 + 10 0.48 + 2 0.08 +

11、 0.033= 47.8 m2g0.2 2 9.8 i代入原式可得所需泵的压头为V 23.182H = 5 + 2g + hW= 5 + 47.8 = 53.3 m2 9.8例 6-7 输水钢管直径 d =1000m,壁厚d =20mm,长 l =800m,钢的弹性模量 E =2 1010Pa,管内水的流速v =1.2m/s试求突然关闭阀门所引起的水击压强和水击周期。0解:水的弹性模量 E = 2 109 Pa,则水击波的传播速度为E0 r1 + E0 dE dc = 1154.7 m/s水击压强p = rcv = 1.3856 106 Pah水击周期T = 4l / c = 2.77 sEx

12、ample E6-1 Oil, withr = 900 kg/m3 andn = 0.00001 m2/s, flows at 0.2m3/s through 500m of 200 mm-diameter cast iron pipe( e = 0.26 mm). Determine ( a ) the head loss and ( b ) the pressure drop if the pipe slopes down at 10in the flow direction.Solution:First compute the velocity from the known flow r

13、ate:V = QpR 2=0.2p (0.1) 2= 6.4 m/sThen the Reynolds number isRe = Vd = 6.4 0.2 = 128000 Thendn0.00001e = 0.26 = 0.0013d200Enter theMoody chart on the right ate / d = 0.0013(you will have to interpolate), andmove to the left to intersect with Re=128000. Read f 0.0225 . Then the head loss is=L V 2 =

14、500 6.42=mAns.( a )h fThereforefd 2g0.02250.22 9.81117h = p + z - z = p + L sin10ofrg12rgforp = rg (h - 500 sin 10o )= rg(117 - 87)= 900 9.81 30 = 265000 PaAns.( b )Example E6-2Water,r = 1.94slugs/ft 3 andn = 0.000011 ft3/s, is pumped between tworeservoirs at 0.2 ft 3 /s through 400 ft of 2-in-diame

15、ter pipe and several minor losses, as shown inFig.E6-1. The roughness ratio ise / d = 0.001.Compute the pump horsepower required.Fig.E6.1 schematic view of example E6-2Solution: Write the steady flow energy equation between sections 1 and 2, the two reservoir surfaces:pV 2pV 2 1 + 1 + z1 = ( 2 + 2 +

16、 z 2 ) + h f + h j - hprg2grg2gWhere hpis the head increase across the pump. But sincep1 = p2andV1 = V2 0 , solvefor the pump head:hp = z 2- z1+ h f+ h j= 120 - 20 V+22g( lL +d K )(1)Now with the flow rate known, calculateV = qVA=0.21 ( 2 ) 2= 9.17 ft/s412Now list and the minor loss coefficients:Los

17、sKSharp entrance Open globe valve 12-in bend Regular 90elbowHalf-closed gate valve Sharp exit0.56.90.250.952.71.0 K = 12.3Calculate the Reynolds number and pipe friction factor:9.17( 2 )Re d= Vdv= 12 = 1390000.000011Fore / d = 0.001,from the Moody chart readl = 0.0216.Substitute into Eq.(1):=9.17 2

18、0.0246(400)h100 +p2 32.22+12.3 12=100 + 84 = 184 ftpump head The pump must provide a power to the water ofV PP = rgq h = 1.94(32.3)1bf/ft 3 (0.2ft 3 / s)(184ft) = 2300ft 1bf/sThe conversion factor is 1 hp=550ft1bf/s. ThereforeP = 2300 = 4.2550hpAns.Allowing for an efficiency of 70 to 80 percent, a p

19、ump is needed with an input of about 6 hp.【习题答案】6-1 V1 = 1.526 m/s, p1 = 28139.3 Pa; p2 = 1119.9 kPa6-2 (1)Re = 281332紊流;(2) Re = 1581层流6-36-4m = 0.023Re1 = 2PasRe 236-5 h f = 8.8 m 油柱6-6 h f = 5.5 mH2O6-7 qv max = 8.25 L/s6-8 qv = 4.25 m3/s6-9 qv = 40.1 L/s6-10p f= 6.49 Pa6-11 h = 0.23 m6-12 (1) p

20、A= pa+ 2 rg(h - 1) ; h = 1mh + l1 + l3(2) qv= 0.00556; h = 1m6-13 a = 1.0586-14 (1)Vmax = 0.36 m/s;(2)h f = 0.423 m 原油柱;(3) t = 5.18 10-4 rp6-15 (1) h f 1 = p ;(2) h f 1 =h f 24h f 226-16qv = 0.105 m3/s6-17H = 7.37 m6-18pv = 24152.97 Pa6-19 H = 9.32 m6-20 hw = 10.79 mH2O6-21 p2 = 100567.923 Pa6-22 H

21、 = 25.7 m6-23 qv = 12.17 m3/s6-24z 2 = 8.653 ,理论值z 2 = 9 (或z 1 = 0.5408 ,理论值z 1 = 0.5625 )6-25 D1 = 210 mm6-26 qv = 0.068 m3/s6-27 p1 = 55035.82 Pa6-28d = 0.6105 m6-29qv1 =2qv286-30 向上流动: pe = -39075 Pa;向下流动: pe = -26475 Pa6-31 H = 2.367 m6-32qv1 = 0.0283 m3/s; qv2 = 0.0967 m3/s; h f= 2.72 mH2O6-33p f= 231.67 Pa6-34 qV = 5.89 L/s6-35 ph = 1514.7 kPa6-36 p1 = 2517.44 kPa6-37hw1-2 = 0.051 mH2O; hw1-3 = 7.95 mH2O

展开阅读全文
相关资源
猜你喜欢
相关搜索
资源标签

当前位置:首页 > 办公、行业 > 待归类文档
版权提示 | 免责声明

1,本文(黏性流体的一维定常流动-习题答案.docx)为本站会员(最好的沉淀)主动上传,163文库仅提供信息存储空间,仅对用户上传内容的表现方式做保护处理,对上载内容本身不做任何修改或编辑。
2,用户下载本文档,所消耗的文币(积分)将全额增加到上传者的账号。
3, 若此文所含内容侵犯了您的版权或隐私,请立即通知163文库(发送邮件至3464097650@qq.com或直接QQ联系客服),我们立即给予删除!


侵权处理QQ:3464097650--上传资料QQ:3464097650

【声明】本站为“文档C2C交易模式”,即用户上传的文档直接卖给(下载)用户,本站只是网络空间服务平台,本站所有原创文档下载所得归上传人所有,如您发现上传作品侵犯了您的版权,请立刻联系我们并提供证据,我们将在3个工作日内予以改正。


163文库-Www.163Wenku.Com |网站地图|