中国石油大学工程力学答案合集1演示教学.ppt_第1页
中国石油大学工程力学答案合集1演示教学.ppt_第2页
中国石油大学工程力学答案合集1演示教学.ppt_第3页
中国石油大学工程力学答案合集1演示教学.ppt_第4页
中国石油大学工程力学答案合集1演示教学.ppt_第5页
免费预览已结束,剩余92页可下载查看

下载本文档

版权说明:本文档由用户提供并上传,收益归属内容提供方,若内容存在侵权,请进行举报或认领

文档简介

2020/6/12,Kylinsoft,Statics-Problems-1,静力学第1章作业/P23-1.1(l)*:,2020/6/12,Kylinsoft,Statics-Problems-2,静力学第1章作业/P23-1.1(g)*:,2020/6/12,Kylinsoft,Statics-Problems-3,静力学第1章作业/P24-1.2(k):,2020/6/12,Kylinsoft,Statics-Problems-4,静力学第1章作业/P27-1.3(c):,2020/6/12,Kylinsoft,Statics-Problems-5,静力学第1章作业/P27-1.3(e)*:,2020/6/12,Kylinsoft,Statics-Problems-6,静力学第2章作业/P58-2.3*:,Solution:,由此得到如下方程组:,解得:,2020/6/12,Kylinsoft,Statics-Problems-7,静力学第2章作业/P60-2.14*:,Solution:,按定义有:,So,expressions(a),(d),(e)arevalid.,2020/6/12,Kylinsoft,Statics-Problems-8,静力学第2章作业/P61-2.20:,Solution:,(a),Invectorform:,2020/6/12,Kylinsoft,Statics-Problems-9,(b),Invectorform:,2020/6/12,Kylinsoft,Statics-Problems-10,+,Solution:,静力学第2章作业/P63-2.28*:,2020/6/12,Kylinsoft,Statics-Problems-11,(a),Solution:,静力学第2章作业/P63-2.30*:,2020/6/12,Kylinsoft,Statics-Problems-12,(b),+,2020/6/12,Kylinsoft,Statics-Problems-13,O,OriginalforcesandcouplecanbereducedtoaforceandacoupleactingatpointO:,静力学第2章作业/P64-2.32:,Solution:,于是得到合力的大小、方向和作用线位置(如图所示):,(或,或,),2020/6/12,Kylinsoft,Statics-Problems-14,+,Solution:,静力学第2章作业/P64-2.34*:,2020/6/12,Kylinsoft,Statics-Problems-15,静力学第3章作业/P85-3.2*:,Solution:,FromtheFBDofthebeaminFig:,+,2m,2020/6/12,Kylinsoft,Statics-Problems-16,静力学第3章作业/P86-3.11:,Solution:,Studyingpersonandladder,drawFBD,(a)x=1.5m,+,2020/6/12,Kylinsoft,Statics-Problems-17,(b),2020/6/12,Kylinsoft,Statics-Problems-18,静力学第3章作业/P87-3.18:,Solution:,0.5m,(1)Studyingentirestructure,FromtheFBDofentirestructureinFig:,+,(2)StudyingmemberAB,FromtheFBDofmemberABinFig:,0.5m,1.6m,+,2020/6/12,Kylinsoft,Statics-Problems-19,(3)StudyingmemberACE,FromtheFBDofmemberACEinFig:,0.8m,A,E,C,0.8m,0.6m,0.6m,+,2020/6/12,Kylinsoft,Statics-Problems-20,静力学第3章作业/P90-3.28(f)*:,Solution:,(1)StudyingmemberCD,FromtheFBDofmemberCDinFig:,显然,本题中在约束A、B、C、D处没有水平方向的作用力,M,C,3m,1m,+,+,2020/6/12,Kylinsoft,Statics-Problems-21,(2)StudyingmemberABC,A,C,1m,2m,1m,FromtheFBDofmemberCDinFig:,+,+,2020/6/12,Kylinsoft,Statics-Problems-22,静力学第3章作业/P91-3.40:,Solution:,(1)FromtheFBDofjointAinFig:,A,1,2,2020/6/12,Kylinsoft,Statics-Problems-23,(2)FromtheFBDofjointBinFig:,B,2020/6/12,Kylinsoft,Statics-Problems-24,(3)FromtheFBDofjointDinFig:,D,1,2,2020/6/12,Kylinsoft,Statics-Problems-25,(4)FromtheFBDofjointCinFig:,C,2020/6/12,Kylinsoft,Statics-Problems-26,静力学第3章作业/P92-3.43*:,Solution:,(1)FromtheFBDofjointDinFig:,D,(1)FromtheFBDofjointinFig:,H,2,3,2020/6/12,Kylinsoft,Statics-Problems-27,Solution:,+,+,+,静力学第4章作业/P111-4.2*:,2020/6/12,Kylinsoft,Statics-Problems-28,静力学第4章作业/P113-4.12*:,Solution:,FromtheFBDofbentpipeandcableinFig:,2020/6/12,Kylinsoft,Statics-Problems-29,无解!?,2020/6/12,Kylinsoft,Statics-Problems-30,Solution:,静力学第4章作业/P113-4.13*:,2020/6/12,Kylinsoft,Statics-Problems-31,静力学第4章作业/P114-4.14(b):,Solution:,S,令形心坐标为(xc,yc),按定义有:,2020/6/12,Kylinsoft,Statics-Problems-32,静力学第4章作业/P115-4.24:,Solution:,已知crucible的密度rc=2000kg/m3,外径R=0.28m,内径r=0.2m;iron的密度ri=7200kg/m3,O,Studyingcrucible,DrawingFBDinFig.,Gi,Gc,+,2020/6/12,Kylinsoft,Statics-Problems-33,2020/6/12,Kylinsoft,Statics-Problems-34,Solution:,x=0,静力学第4章作业/P116-4.27*:,2020/6/12,Kylinsoft,Statics-Problems-35,静力学第5章作业/P131-5.2:,解:,假设系统是静力平衡的,先研究圆柱,有,得,再研究方块,有,得,而,2020/6/12,Kylinsoft,Statics-Problems-36,Discussion:,1.方块会不会先翻倒?,2.如果圆柱和方块的接触面不光滑,会怎样?,x2,x2=?,2020/6/12,Kylinsoft,Statics-Problems-37,Solution:,总体分析:,分析木条:,圆盘分析:,解之得:,N,f,f,f,C,B,A,.,=22.06,=,=,达到最大静摩擦力时:,解之得:,静力学第5章作业/P132-5.10*:,2020/6/12,Kylinsoft,Statics-Problems-38,静力学第5章作业/P132-5.12:,解:,假设系统是静力平衡的,先研究桩子CBD,有,再研究杆AB,有,2020/6/12,Kylinsoft,Statics-Problems-39,只有当fAfAmax或fBfBmax时,杆AB才能移动,由以上计算结果可知,当P6300(N),杆AB在A点处开始移动,2020/6/12,Kylinsoft,Statics-Problems-40,静力学第5章作业/P133-5.18*:,Solution:,因此:,2020/6/12,Kylinsoft,Statics-Problems-41,Solution:,木块翻转临界时:,滑动时:,静力学第5章作业/P133-5.19*:,2020/6/12,Kylinsoft,Statics-Problems-42,当P=600lb时:,当P=200lb时:,Solution:,静力学第5章作业/P134-5.22*:,2020/6/12,Kylinsoft,MOM-Problems-43,第六次作业/P34-1.1(b):,Solution,N1=P,N2=0,N3=P,2020/6/12,Kylinsoft,MOM-Problems-44,第六次作业/P34-1.6:,Solution,研究活塞杆,有,研究右挡盖,有,得,2020/6/12,Kylinsoft,MOM-Problems-45,第六次作业/P34-1.7*:,Solution,研究节点B,有,研究杆BC,有,研究杆AB,有,取,2020/6/12,Kylinsoft,MOM-Problems-46,第六次作业/P35-1.13*:,Solution,根据题意列出方程组:,解得,总伸长为,2020/6/12,Kylinsoft,MOM-Problems-47,第六次作业/P37-1.14*:,Solution,B,C,A,(1)AformulaforthedownwarddisplacementdCofpointC,P,P,(2)TheelongationdBoftheentirebar,2020/6/12,Kylinsoft,MOM-Problems-48,(3)Theratioroftheelongationoftheupperhalfofthebartotheelongationofthelowerhalfofthebar,Theelongationoftheupperhalfofthebar,Theelongationofthelowerhalfofthebar,So,2020/6/12,Kylinsoft,MOM-Problems-49,第六次作业/P37-1.21:,Solution,(1)静力平衡方程:,研究右挡板,有,(2)变形协调方程:,(3)求解方程组:,2020/6/12,Kylinsoft,MOM-Problems-50,P,第六次作业/P37-1.23*:,Solution,P,(1)Equationofequilibrium,(2)Equationofcompatibility,(3)Force-displacementrelations,得补充方程,2020/6/12,Kylinsoft,MOM-Problems-51,解得,有,2020/6/12,Kylinsoft,MOM-Problems-52,第六次作业/P37-1.24*:,Solution,变形过程中3根杆的长度始终满足下面的关系:,而3根杆的长度变化满足下面的关系:,(1)静力平衡方程:,研究节点A,有,(2)变形协调方程:,2020/6/12,Kylinsoft,MOM-Problems-53,(3)求解方程组:,2020/6/12,Kylinsoft,MOM-Problems-54,将A点的位移分量向各杆投影.得,变形关系为,(4)讨论:3根杆长度变化关系的另一种求法:,2020/6/12,Kylinsoft,MOM-Problems-55,RB,RA,第六次作业/P37-1.26:,Solution,A1,A2,(1)Equationofequilibrium,(2)Equationofcompatibility,RB,RB,(3)Force-displacementrelations,得补充方程,2020/6/12,Kylinsoft,MOM-Problems-56,解得,2020/6/12,Kylinsoft,MOM-Problems-57,材料力学第2章作业/P58-2.1(b):,Solution,2020/6/12,Kylinsoft,MOM-Problems-58,材料力学第2章作业/P59-2.11:,Solution,(1),对于AB段,,由强度条件得,由刚度条件得,2020/6/12,Kylinsoft,MOM-Problems-59,取,由强度条件得,由刚度条件得,对于BC段,,取,(2),取,(3),齿轮1安放在齿轮2、3中间。,2020/6/12,Kylinsoft,MOM-Problems-60,材料力学第2章作业/P59-2.14:,Solution,方法一(传统法):,1.解除某些约束,施加相应约束反力,使之成为静定基;,2.扭矩与变形协调方程:,得TB=5T0/4,3.外扭矩3T0和T0作用处的转角分别为:,=,2020/6/12,Kylinsoft,MOM-Problems-61,材料力学第2章作业/P59-2.14:,Solution,方法二(船长法):,1.解除约束,施加约束反力;,2.扭矩与变形协调方程:,右起第一段:TB右起第二段:TB-T0右起第二段:TB-4T0,得TB=5T0/4,3.可见,右起第一段和第二段的扭矩都大于0,最大转角发生在外扭矩3T0作用处:,2020/6/12,Kylinsoft,MOM-Problems-62,材料力学第3章作业/P72-3.1(c):,Solution,对于1-1截面,有,对于2-2截面,有,2020/6/12,Kylinsoft,MOM-Problems-63,补充:内力图,-,-,2020/6/12,Kylinsoft,MOM-Problems-64,Shear-ForceandBending-MomentEquations,材料力学第3章作业/P73-3.2(a):,Solution,2020/6/12,Kylinsoft,MOM-Problems-65,(2)Shear-ForceandBending-MomentDiagrams,-,(3)MaximumShearForcesandBendingMoments,2020/6/12,Kylinsoft,MOM-Problems-66,材料力学第3章作业/P73-3.3(b)*:,Solution,控制截面法?,2020/6/12,Kylinsoft,MOM-Problems-67,Solution,材料力学第4章作业/P90-4.6*:,1.求约束反力,2.求弯矩,作出弯矩图,3.求许用载荷,由强度条件得,2020/6/12,Kylinsoft,MOM-Problems-68,材料力学第4章作业/P91-4.8:,Solution,AT-beammadeofcastironinpurebending.Knowingtheratiooftensileallowablestresstocompressiveallowablestressisst/sc=1/4.Determinethereasonablewidthboftheflange.,2020/6/12,Kylinsoft,MOM-Problems-69,材料力学第4章作业/P91-4.13:,Solution,1.求剪力和弯矩,作出剪力图和弯矩图,2.根据胶合面强度条件求P,整个截面都是危险截面,考虑剪应力互等定理,有,2020/6/12,Kylinsoft,MOM-Problems-70,3.根据截面剪应力强度条件求P,整个截面都是危险截面,有,4.根据截面正应力强度条件求P,A截面是危险截面,有,5.综上所述,取,2020/6/12,Kylinsoft,MOM-Problems-71,材料力学第5章作业/P110-5.3(c)*:,Solution,1.求约束反力,2.求弯矩方程,2020/6/12,Kylinsoft,MOM-Problems-72,3.求挠曲线方程:,代入边界条件:,得:,最大挠度:,两端转角:,中间挠度:,取合理解,2020/6/12,Kylinsoft,MOM-Problems-73,材料力学第5章作业/P111-5.8:,Solution,ThecantileverbeamshowninthefigurehasmomentsofinertiaI1andI2inpartsACandCB,respectively.(a)Usingthemethodofsuperposition,determinethedeflectiondBatthefreeendduetotheloadP.(b)DeterminetheratiorofthedeflectiondBtothedeflectiond1atthefreeendoftheprismaticcantileverbeamwithmomentofinertiaI1carryingthesameload.,B,A,C,(a),B,C,A,2020/6/12,Kylinsoft,MOM-Problems-74,B,A,C,B,C,A,2020/6/12,Kylinsoft,MOM-Problems-75,B,A,C,(b),2020/6/12,Kylinsoft,MOM-Problems-76,B,A,C,Discussion,Useenergymethod,2020/6/12,Kylinsoft,MOM-Problems-77,材料力学第5章作业/P111-5.9:,Solution,1.解除某些约束,施加相应约束反力,使之成为静定基;,2.变形协调方程:,=,查表得,2020/6/12,Kylinsoft,MOM-Problems-78,3.求其它约束反力:,2020/6/12,Kylinsoft,MOM-Problems-79,材料力学第5章作业/P112-5.13*:,Solution,Thebars1and2havethesametensilerigidityEA.(1)IfthebeamABisconsideredasrigid,determinetheinternalforcesinthetwobars.(2)IfthebeamABisconsideredasdeformablewithbendingrigidityEI,determinetheinternalforcesinthetwobars.,(1)thebeamABisconsideredasrigid,P,P,(a)Equationofequilibrium,(b)Equationofcompatibility,2020/6/12,Kylinsoft,MOM-Problems-80,(1)thebeamABisconsideredasrigid,P,P,(a)Equationofequilibrium,(b)Equationofcompatibility,(c)Force-displacementrelations,得补充方程,解得,2020/6/12,Kylinsoft,MOM-Problems-81,(2)thebeamABisconsideredasdeformable,P,(a)Equationofequilibrium,(b)Equationofcompatibility,(c)Force-displacementrelations,得补充方程,解得,2020/6/12,Kylinsoft,MOM-Problems-82,1.危险点位于圆轴固定端横截面的最上处和最下处(A点和B点),材料力学第6章作业/P135-6.1(d):,m,d,Solution:,忽略横力弯曲剪力的影响,2.用单元体表示危险点的应力状态,3.用应力圆表示危险点的应力状态,(,),(-,),(0,-),A,B,A点:,或,B点:,或,2020/6/12,Kylinsoft,MOM-Problems-83,材料力学第6章作业/P135-6.3(d):,40,20,40,如右图所示单元体,画出对应的应力圆,Solution,tmax,(-40,-40),(-20,40),1.主应力和主方向,s3,s1,11.23,71.23,2.如图所示在单元体上画出主平面方向,52.02,3.最大剪应力,2020/6/12,Kylinsoft,MOM-Problems-84,材料力学第6章作业/P135-6.4(b)*:,30,30,50,20,如右图所示单元体,画出对应的应力圆,Solution,s1,s2,tmax,(30,-20),(50,20),60,(52.32,-18.66),a=30,2020/6/12,Kylinsoft,MOM-Problems-85,材料力学第6章作业/P136-6.7*:,Solution,30,如右下图所示,在A点取单元体并进行应力状态分析,a=120,Atestofthinwalledtubeisshowninthefigure.IftheloadsareaconcentratedforceP=20kNandatorqueT=600Nm.Thediameterofthetubeisd=50mm,thicknessisd=2mm.(1)DeterminethenormalandshearstressesontheinclinedsectionatpointA.(2)DeterminethemagnitudeandorientationoftheprincipalstressesatpointA.(Drawstresselement.),2020/6/12,Kylinsoft,MOM-Problems-86,(2),(61.21,-70.63),(0,70.63),s3,s1,66.57,33.29,(1),2020/6/12,Kylinsoft,MOM-Problems-87,材料力学第6章作业/P136-6.11:,Solution,Whenatrainpassthroughasteelbridge,thestrainstestedbyinstrumentareex=0.0004,ey=-0.00012atpointA.FindthenormalstressesindirectionsxandyatpointA.(E=200GPa,m=0.3),2020/6/12,Kylinsoft,MOM-Problems-88,材料力学第6章作业/P137-6.17*:,Solution,薄壁上任意一点都是危险点,在薄壁上任一点A取单元体并进行应力状态分析,Athin-walledtubeshowninthefigureismadeofcastiron.KnowingitsoutsidediameterisD=200mm,thicknessofthewallist=15mm,theinnerpressureisp=4MPa,thecompressiveforceisP=200kN.Theallowabletensileandcompressivestressesofcastironarest=30MPaandsc=120MPa,respectively.Examthestrengthofthethin-walledtube.,2020/6/12,Kylinsoft,MOM-Problems-89,由上可知,由第一强度理论可知,强度满足,由第二强度理论可知,强度满足,由莫尔强度理论可知,强度满足,2020/6/12,Kylinsoft,MOM-Problems-90,材料力学第6章作业/P137-6.18:,Solution,1.求A点所在横截面的内力,2.在点A处取单元体并进行应力状态分析,AcantileverbeamofrectangularcrosssectionissubjectedtoaconcentratedloadP=120kN,actingatthefreeend.Thebeamhaswidthb=100mm,andheighth=20

温馨提示

  • 1. 本站所有资源如无特殊说明,都需要本地电脑安装OFFICE2007和PDF阅读器。图纸软件为CAD,CAXA,PROE,UG,SolidWorks等.压缩文件请下载最新的WinRAR软件解压。
  • 2. 本站的文档不包含任何第三方提供的附件图纸等,如果需要附件,请联系上传者。文件的所有权益归上传用户所有。
  • 3. 本站RAR压缩包中若带图纸,网页内容里面会有图纸预览,若没有图纸预览就没有图纸。
  • 4. 未经权益所有人同意不得将文件中的内容挪作商业或盈利用途。
  • 5. 人人文库网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,对用户上传分享的文档内容本身不做任何修改或编辑,并不能对任何下载内容负责。
  • 6. 下载文件中如有侵权或不适当内容,请与我们联系,我们立即纠正。
  • 7. 本站不保证下载资源的准确性、安全性和完整性, 同时也不承担用户因使用这些下载资源对自己和他人造成任何形式的伤害或损失。

评论

0/150

提交评论