NASA NACA-ARR-L6A05-1946 Charts for critical combinations of longitudinal and transverse direct stress for flat rectangular plates《平面矩形板纵向和横向直接应力临界组合图》.pdf
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1、i i_L_-r_ CA$ F,COPYAm_ No. _AO_NATIONAL ADVISORY COMMITTEE FOR AERONAUTICSIrl RTIMl RI: P()RTORIGINALLY ISSUEDMarch 1946 asAdve_ce Restricted Repart Tf:_05CHARTS FOR CRITICAL COMBINATIONS C_ LONGITD)INALAND TRANSVERSE DIRECT S_EqS FOR FLATRECTANGULAR PLATESBy Charles Libove and Manuel SteinLangley
2、Memorial Aeronautical LaboratoryLangley Field, Va.FILE COPYNOT REPRODUCIBLEWASHINGTONNACA WARTIME REPORTS are reprints of papers originally issued to provide rapid distribution ofadvance research results to an authorized group requiring them for the war effort. They were pre-vlously held under a sec
3、urity status but are now unclassified. Some of these reports were not tech-nlcally edited. All have been reproduced without change in order to expedite general distribution.Reproduced byNATIONAL TECHNICALINFORMATION SERVICEU S Deportment of CommerceSprlngfied VA 22151L - 2Z4/Provided by IHSNot for R
4、esaleNo reproduction or networking permitted without license from IHS-,-,-Provided by IHSNot for ResaleNo reproduction or networking permitted without license from IHS-,-,-., l_: ; T , _,r“ 7_,_(_i_;so.t,b,:_ skin cf :_n _:12:?,.,un.-_“r in r“ ;-:t is sub.-.-_:-.Fr:,! b ? Sqr , “ “ “ “ “ -, ,_n,_tz_
5、n,-, ,:,f s,tres:_, _tt_nLi n _._:s been4-/: V,%_ “; f“_-. “_,. _,.,_,.p._“ I p-“ r, i R.,k!:L_S ,:ii6ri :,C:Z_*“ ,;l_.tZ_:_: ,;tPeS.S :S :_C_S_:lt :,: lstresnes can be evalueted, the effect of the combinationshould be considered in investigating the stabilit F of theplate.The energy method is used
6、to derive 5ntersctionequations that define tl_e critical combfnations of lonzi otudinai and transverse direct stress for isotropic flatrectangular plates with the following four cases of edgeconditions:CO.S e(b)(o)(d)Long edsesSimply supportedSimply supportedClsmpedClampedShort edgesSimply supported
7、ClampedSimply supportedClampedCharts based upon the inter_ction equations are presentedfor these four cases.The solution obtained for case (a) is exact. Forthe other three cases the s_7utions obtained ere approxi-m_,te and, as is cheracteristc of the energy method,tmconservative. Comparisons with kn
8、own exact solutionsand lower-limit solutions indicate, however, tho t theerro_,_ in the present results are generally small.SY;4BOLSbtW7en_th of ol_tewidth of o!s_te (bt c !_hir-.: -_ t,:.,-iuti:zns t,_,_,_ v:hicb. _ tLe int, e_aet_ _Cl_tpt; _ are 1-_sc: i:e r.,“Vt; _ _lff. tDpcn_!x m:e ; f,_r_: , s
9、,:;_o !.:. _“ ,-,_-, :rz, i (a.:_,:;,s (_o)t,! !_ 1“(- r.j_ :)IL b_.t _“- . . ,_, . “ ._ _ i _ “ ., -(c), anJ (d) ,.r:. c -,:.+ ,r:._ ;1 .r;_ _ tO*u . .1., s ,I _ _ o .2,_ I uC_e SS_ ,_“_._,._. sr_ ,:irt “_. ?.-i s ,sT.r_c i krla/_ %o rcpp,Jsc_= aqt,.,;r i. _it _ _2 %);P -:aPe !llSEf “_,“ :. rSb-O t
10、 ecaus-, all- _ “_S =_u,-_l, s-._-_,lC(SIZ _i.L;P Lz S_:.I 0SS OOTIb_“ IiO-t, io: in *./.,.:,oh t!.:o tr:nzve: 3_- _.!z,.:lCb stne:.:s q, _ s one-Jt, “ _“ p, t%o :T:u:; .:.t ,z :.c!, - = := .s icun_ alorv: tKe,!- 7,?in.e ; - 2 in .:i .,_:,_ ! glue v:- iue :Tf :;: _ _:s p?int, 7 p.:_ t_c r,_Pres.O:C_
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