化学工程基础习题答案

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化学工程基础习题答案

第二章流体流动与输送

5、解:

0013.60.22.181.25gHgRgRHmg

001.252.181.701.6gHgRHRm

6、解:

1001223113.60.1302.210.80()2(2.210.2)8006.051044gHgRRHmmdHhkg

10、解:列柏努力方程

221122122212121222210,20,0,12.3213.382ffpupuzzhgggguzmzppuhgug

解得

123.44ums

22313120.13.440.0271.62min44vqdumsm

11、解:列柏努力方程

2211221222122121212212212222212122()20()22()2iiipupuzzggggppuuzzggzzpppuughuuuuhgg

1122112221700/360014.0(0.21920.006)441700/360026.7(0.15920.0045)440.037737.7vvqumsdqumsdhmmm

12、解:列柏努力方程

221211222212212121122312222()()20,215.8()114.5()()114.5102uuzgpzgpgguupzzgpzzpkPakPauup绝压表压

1122112220.5/36000.4420.02440.5/360019.70.00344vvqumsdqumsd

22321000(0.44219.7)104.51079.42pkPa

17、解:列柏努力方程

221122122221212121121122222()216,0,06/36002.91(0.03220.0025)44efefvpupuzHzhggggppuuHzzhggzzmppuqumsd

900弯头阻力系数ξ=0.75

全开截止阀阻力系数ξ=6.0

5312302.910.027Re1.01109.510ud,查图得到λ=0.026

22802.91(60.7546.0)(0.0264.524)45.5520.0272fluhmdgg

2222121212.91()16045.5561.9822efppuuHzzhmggg

18、解:列柏努力方程

221122121212122150,0,15ffpupuzzhggggzzmppuh忽略动能

假设流体流动类型为层流

2222222222520010.2224.251040.43415efVflluuuhdgdgdquddhd

解得0.111dm

核算

1223.454ReVqumsdud

22、解:列柏努力方程

220022022220202020020112222()26.5,0,05/36000.630.05344efefvpupuzHzhggggppuuHzzhggzzmppuqumsd

由连续性方程得到

221212220.530.631.05/0.41duumsd

113223112218300.630.053Re1222501018301.050.041Re15765010640.052Re640.041Reudud

900弯头阻力系数ξ=0.75

全开截止阀阻力系数ξ=6.0

三通阻力系数ξ=1.0

22112212121222(40.7526.01)[(300200)50.75]22400.63251.05 (0.0523121)[0.041(300200)3.75]0.05320.0412 1.122.773.89fffluluhhhdgdgggm222020202()21.05 =6.5+3.8910.452efppuuHzzhggmg

10.455/360018309.814340.4340.6VHeqgPWkW

24、解:根据汽蚀余量的定义

211110002210102212101.32573.328.0252()29.810.75(13.61)0.751010.038102.050.084VappuhgggpkPagRuCmsduumsd

查表得到pV=2.3346kPa

代入上式解得

2231128.0252.33462.05102.8429989.8129.81Vappuhmggg

第三章 传热过程

2、解:⑴

2111121222213330.250.1791.40.130.8670.150.200.250.8RmKWRmKWRmKW

⑵22328202606460.867TTqWmR

23112313123646116820260560162838TTTqWmRRRRRTKTKTKTK

8、解:热量衡算

36111222216213226216000()3.010(485155)1.65103600()1.65105037658003.141036001.6510514(485376)(15550)302mpmpmpmmQqcTTWQqcttQttqcQKAtQKWmKAt

10、解:

⑴热量衡算:

乙醇冷凝热3511500/3600880101.2210mQqrW

乙醇冷却热3421112()500/36002.810(78.530)1.8610mpQqcTTW

水的用量

122231541122231()1.22101.86101.67()4.2(3515)mpmpQQqcttQQqkgsctt

冷却器水出口温度的计算

222214221322()1.86101517.71.674.210mpmpQqcttQttqc

冷却器面积的计算

以外表面为基准

21112211380124111700201000(78.517.7)(3015)33(78.517.7)ln(3015)mKWmKddtK

2142211.86101.4838033mmQKAtQAmKt

冷凝器面积的计算

211122116731241113500201000(78.535)(78.517.7)51.7(78.535)ln(78.517.7)mKWmKddtK

1252121.22103.5167351.7mmQKAtQAmKt

总面积2121.483.514.99AAAm

⑵14.99333.140.0242Andl根

16、解:

361162221661232214000109251.03103600()1.03101.03101.031012.3()4.1810(4020)mmpmpQqrWQqcttWqkgsctt

⑵因为酒精冷凝为相变传热,因此并流或逆流没有差别

⑶1212()()(7820)(7840)47.3()7820lnln7840()mTtTttTtTt℃

第五章 吸收

6、解:⑴

424211341.341001111.3427363.84101.02103.6610YyxYEmpmKkkKkmolms

⑵气膜阻力3214112.60103.8410ymskmolk

液膜阻力

22121.341.31101.0210xmmskmolk

332.610==0.9522.610131气膜阻力总阻力

气膜阻力远大于液膜阻力,因此为气膜控制

⑶*1.340.050.067ymx

*0.10.9520.10.0670.06860.06860.05121.34iiiiiyyyyyyyxm

9、解:

1220.08/1140.0930.08/114(10.008)/135)0.0081140.000950.0008/114(10.0008)/135)0XXY

最小汽液比的计算

12*min12121210.0930.000951.980.0930.5031.985.945.940.0930.0009500.01555.94XXVLYYVLXXVLYYY

**1122*11*2212()()(0.50.0930.0155)(0.50.000950)0.0073(0.50.0930.0155)lnln(0.50.000950)0.015502.050.00730.82.051.64mOGmOGOGYYYYYYYYYYYNYHHNm

12、解:⑴根据已知条件可得

12120.01(1)0.0010YYYX