Proiect: PN-III-P4-ID-PCE-2020-1988
Proiect: PN-III-P4-ID-PCE-2020-1988
Contract: PCE 168/2021
5$3257 ܇7,,1܉,),&
privind implementarea proiectului vn perioada ianuarie-decembrie 2021
,QJLQHULD PDWHULDOHORU FHUDPLFH SRUR-, DpirVoeHlec trIiciăcuUă S DSOLFDаLL GH FROHFWDUH GH HQHUJLH
Rezumat etapăI:
ÌQ DFHDVWăD XS UILRPVăW HUWHD܊DSLOdOiLn Hp]laDnuWl dHe reaDlizFareWaLpYroiLecWtulăui: A1.1-3 care au conVWD1W) dezvvoQltarea de modele combinate pentru simularea GH PLFURVWUXFWXUL S UROXOXL DFHVWRUD DVX2S) 6UWDX GULăXVOS XLQPVSXDOiFXGWLHX OSFXLkLHP ]SGR LHVOWHUFLW
UăVSXQVXOXL GLOHOFHWFUWLUFL F 3 S(L H ]܈RL SWLXUQRDHELOcLonWtinDuaWreHv QS HQ 2022). A1.3 Proiectare de microstructuri ceramice piezo-/piroelectrice, folosind modele teoretice, cu FOM vPEXQăcWonătin܊uaLreWvHQ ; au fo st vndeplinite DFWLYA1L.4W-5 ăde܊sLinteză܈L FDUDFWH PLFURVWUXFWXUDOă D SXOEHULORU SH ED]ă GH VROX܊
perovskit pHQWUX IRORVLUHD DFHV, iaWr dRinUpuDlb erFileDR EP܊DLaWuQUpXroLWduFHseH ce raImiHci URH poroase făUă 3E FX GLIHULWH WcLonStinXuaUre L20 22G). ÌHQ FFRDQGHLUFWXWi ăAOL1܊ Y.6L,DLs-FWWDLWYH a efectuat pURLHFWDUHD G܈HL GSLUVRSGRX]FLHWULHYDH H[SHULPHQWDOH SH
LPSOXVXULORU WHUPLFHta rea܈eLne rgiPei HdiFn DdiQferLiteFmHed ii;SAH1.Q7 PDQDJHPHQW ܈ LD GULHV]HXPOLW.QDWUHHORU RE܊LQXWH
WCoUorXdo narFe, ROH
DHVFULHUHD úWLLQĠLILFă úL WHKQLF
FX SXQHUHD vQ HYLGHQĠă D UH]XoObiWectDivWeloHr O- seRvUor inHdiWcaDSHL UH]XOWDWHOH úL PRGXO GH GLVHPLQDUH
A1.1 'H]YROWDUHD GH PRGHOH FRPELQDWH SHQWUX VLPX DFHVWRUD DVXSUD UăVSXQVXOXA1L.2 6SWLXHG]LRXHOO HLFPWSUDiLFGFWH X vOFQXk LP S HOHFWULF DVXSUD UăVSOXHQFVWXUOLXFL G3L H(O H F܈WLU LWFX Q DSELLHO]LRW D
(activitatea YD FRQWLQAX1.D3 P rovieQcta re de m icr os tru ct uri ceramice piezo-/piroelectrice, folosind PRGHOH WHRUHWLFH FitaXtea Y)D2 0F RvQPWELXQQXăDW ăv܊QL W H D F WLY
Descrierea sistemelor ceramice dense prin simulari Monte-Carlo
Pentru a descrie prin simulăUL UROXO PLFURVWUXFWXULORU SRUR܈Di VH
IHURHOHFWULF vQ FHUDPLvnFtkiLm icrSosRtruUctRuriDceVraHmi ce foDlosXin d mIetRodVe MWo ntJe HQH
Carlo utilizkQG PRGHOXO 3RWWV $FHVWD D IRVW LQL܊LDO S
[1] SHQWUX GHVFULHUHD VWUXFWXULORU GH GRăPVHWQăLUL vGQH
posibile. 6LVWHPXO FRQVLGN xHNUsDpinWi a vkHndVHWamHilt onRian ulU: H܊HD GH
ܪൌെσߜௌௌೕ, (1)
unde ߜௌௌೕUHSUH]LQWă VLPEROXO OXܵLൌ ܵ.)UVRDQXH F ܵN H് UܵG) D[2܈]F. LLăa paLsuDl
YD
LQL܊LDO VH DWULEXLH YDORUL DOHDWRULL VSLQLORU WRWDO DO VLVWHPXOXL Vă V[F3] DXGWăL O L3]UDRWFăH GSXUUHDV XVSWXDQQHG D VSLQ ܈L DWQURLE XYLDUOHRDU LX Q H'LDFă DFHDVWă VFKLPEDUH G
VLVWHPXOXL PRGLIÌLn
FcazDcU
onHtrDar, scHhimVbWareHa estDe FtoFtu܈HLS WDFWFăH S WDWă
probabilitate mai mică SHQWUX D QX SHUPLWH Vi inLteVrmWedHiarPe)X. POrocXedLur a eVsteă VH UHSHWDWă ăUG HP DXUQH QGXHP RUL SkQă FkQG VH DWLQJH VW 7LPSXO vQN xFNDYUHHU LDIXL FOăRUFL DOH XVQWLăWUDLWLH DG HG HV SWLLQP SU HvSQU H
܈L VH 0Q&R6W H D0]RăQWH &DUOR 6WHS $FH[4@VW ܈LP RvGHQO F[D2] GUIXROV SHQWUX D JHQHUD PLFURVWUXFWXUL FHUDPLFH SROLF
microstructurăFHUDPLFă YLUWXDOăD JSUUDRQFXHOGHXOURDU GHHV WFHU HI܈L-WaQHDUOHL DWLQV GLPHQVLXQHD PHGLH GRULWă D JUDQXOHORU
/D SDVXO -a XutiUlizPatăteWoriRa ULa nd au-VGinzburg-Devonshire (LGD) [5] pentru a simula IRUPDUHD GRPHQLLORU IHURHOSHUFHWFUXLPF H܈ Lv QH YFRHOUXD܊PLLDF ăG
௬
ଵଵ ௫
௬
ଵଶ௫ ௬
ଵଵଵ௫
௬
ଵଵଶ௫ ௬
௬ ௫
HOHFWULF 3RODUL]D܊LD VSRQWDQă HVW-DHev onGshHireV: FULVă I
ଵଵ ௫
ܨൌߙ
൫ܲଶܲଶ൯ߚ ൫ܲସܲସ൯ߚ ܲଶܲଶߛ
൫ܲܲ൯ߛ
൫ܲସܲଶܲସܲଶ൯, (2)
XQGH Į ȕ Ȗ VXQW ܲ௫F܈RܲL௬Q UVHWSDUQHW]HL QGWHă PSDUWRHLUHLFD܊OL L OLHD UY HF D[HORU FULVWDORJUDILFH ÌQ ID]ܲDൌ Ͳ S DULDHUO HvFQW UFLHFDă HQHUJLD HVWH PܲL്QͲL DPOăH SSHRQOWDUUXL ]YD܊OLRHULL DYkQG RULHQW 3HQWUX D GHVFULH IRUPDUHD GRPHQLLORU IHURHOHF HQHUJLHL SHUH܊LORU GH GRPHQLL
ܨீ ൌ݃
൫ܲଶ ܲଶ ൯݃ ܲ ܲ
݃ ሺܲ
ܲ ሻଶ+݃ǡሺܲ
െܲ ሻଶ, (3)
ଵଵ ௫ǡ௫
௬ǡ௬
ଵଶ௫ǡ௫ ௬ǡ௬
ସସ ௫ǡ௬
௬ǡ௫
ସସ ௫ǡ௬
௬ǡ௫
unde parametrii ݃VXQW FRQVWDQWH ܲGǡH U HPSDUWH]ULLQDWOă GLHDUiUDL YQSDRRWOD ܊UFLRD] ID܊ă GHj G3LUULHQF ܊XLUDP DUH HQHUJLD OLEHVUWăă DH WVDLSVăW HFPDX D GRXă FܨR௧Q௧WൌUσሺLܨEXܨ܊ீሻL, uLnd e ܨ܈ܨLீ VH HVWLPHD]ă SHQWUX ILH GLVFUHWL]DUH ÌQ FHUDPLFă RULHQWDUHD FHOXOHOR
URWD܊LHL GLQ LQWHULRUXO JUDQXOHORU ID90܊o. ăUn ghGiuHl d e VLV URWD܊LH DO FHOXOHORU HOHPHQWDUH D IRVW DVRFLD
Xxxxs.
3HQWUX D VLPXOD FUH܈W-DH USHRDU QGLRWP HGQHL LODR UR IFHRUQRIHLO RULHQWăUDLO HD OSHRDOWDRUULL]LD ܊LHL FHOXOHORU HOHPHQWDUH FHOXOHORU GH GLVFUHWL]DUH VH DMXVWHD]ă VXܨFFHV SHQWUX ILHFDUH FHOXOă ܲ௫G܈HLܲ ௬ GQLXV FVUXHQWWL ]SDUURHL H F܊RLPLSORHQ
FRQVLGHUDWH FD UHIHULQ܊ă GHFkW SHQWUX JUDQX FHOHODOWH JUDQXOH DFHVWH FRPSRQHQWH VH FDOFXO
௫
௬
௬
௫
௬
ܲ௫ൌܲכ ሺߙሻܲכሺߙሻ܈ܲL ൌെܲכሺߙሻܲכ ሺߙሻ, (4)
unde ܲכ܈ܲLכ UHSUH]LQWă SURLHF܊LLOH3 HSQRWOUDXU LF]DDO܊FLXHOLX OS HG HDI
௫ ௬
FDUH VXQW desHcrVierHeaQră܊spLunDsuOluiHp iezvoelQec tric vQ IHUR-DH OHLFPWSUOLHFPLH QWVDW 0RQWH &DUOR ED]DWă SH WHRULD /*' JHQHUDOL]DWă
termeni:
ܨ௧௧ൌσሺܨܨீܨ௧ܨ௦ሻǡ௧
(5)
Pentru descrierea efeFWHORU PHFDQLFH VH ܊LQH FRQW GH FXSO
ଵଶ௬
௬ǡ௬
ଵଵ௬
ଵଶ௫
௫ǡ௬
௬ǡ௫
ସସ௫ ௬
ଵଵ
௫ǡ௫
HODVWLFH ORFDOH SUHFXP úL HQHUJLkDx2 /2)H: ODVWLFă VSH
ଵଵ௫
ܨ௦ൌ௧െݑ௫ǡ௫൫ܳ
ܲଶܳ
ܲଶ൯െݑ
൫ܳ ܲଶܳ
ܲଶ൯െ൫ݑ
ݑ ൯ܳ
ܲܲ ܥ ൫ݑଶ
ݑଶ ൯Ȁʹܥ ݑ ݑ
ܥ ൫ݑ ݑ
ଶ
, (6)
௬ǡ௬
ଵଶ௫ǡ௫ ௬ǡ௬
ସସ ௫ǡ௬
௬ǡ௫൯Ȁʹ
unde parametrii Q úLC UHSUH]LQWă FRQVWDQWH GH PDWHULDO F elastice). Variabilele ݑ௫ úLݑ௬ VXQW GHSOODHV ăDUOLHO HQ ROGRXFUDLORU GLQ UH܊ SR]L܊LLOH ORU FRUHVSXQ]ăWRܲD௫UൌHܲ௬ ൌXͲሻQ, iHar Lter meVniWi ݑă௫ǡ௫U, ݑL௫ǡ ௬, Qݑ௬Hǡ௫SRO úݑL௬ǡ ௬VXQW DOXQJLUL UHODWLYH DOH FHOXOHORU GH GLV GHIRUPDWă OLSVD SRODUL]D܊LHL VSRQWDQH
3HQWUX FDOFXOXO GHSODVăULORU ORFD-Oa Hdez vovltaQt o WRD
SURFHHGUXDUWăL YLăW 0RQWH &DUOR ED]DWă SH SULQFLSLXO
VXFFHVLY GHSODVăUL QRL DOH QRGXܨULO௦. R௧PeUb azaFpRroUcedHurVii SXQ GHVFULVH DQWHULRU DH QILRLVOWR UP RIQHLUWRHUOLH]FDWUăL FHHY Răr܈Oui LX ܊DLX
QRG GLQ UH܊HDXD GH GLVFUHWL]DUH SHQ, pWrinUmXin imDiz areHa YDO HQHUJLLORU HODVWLFH vQ XUPăWRDUHOH VLWXD܊LL
L GRPHQLL ÄDV JURZQ´ IRUPDWH LQL܊LDO vQ
LL vQ WLPSXO GHVFULHULL FXUEHL GH SULPă S
LLL vQ WLPSXO SDUFXUkJPHSUേXLܧO.L FLFOXULORU GH K
)LJ 6WUXFWXUD GH GRPHQLL LQLаLDOă ÄDV JU
Fig. 2 Structuri de GRPHQLL ЮL GHIRUPăUăLU LO R0FRDQOWH & DUUHO]RX OvWQD DOH SDUFXUJHULL XQXL FLFOX GH KLVWHUH]LV FRPSO
ЮL GHIRUPăULL UHODWLYH 6 ( FDOFXO
Descrierea sistemelor ceramice cu porozitate
3URFHGXUD GHVFULVă DQWHULRU SHQWUX FHUDPLFL DYkQG SRUL L]RWURSL GH IRUPă VIHULFă VDX SRUL
SDUDOHHOU SFHkQWG L܈FLX OSDU SH D[D OXQJă D SRUL-aOgeRneUrat unSHQW VLVWHP FHUDPLF FX DFa7H8%H, Dda܈r cLu miGcroHstrQucVtuLri WdifDeriWte:H(i ) pUorHi izOotDropWi LdeYă G IRUPă VIHULFă -D OLXLQ J XSOR OUHFLFk WPDUSOLXFOQ XJLDL S܊OHLL FGDHW ܈L UHVSH OXQJă SHUSHGLFXODUă SH FkPSXO HOHFWULF DSOLFDW
ÌQ )LJ VXQW SUH]HQWDWH UH]XOWDWHOH VLPXO SHQWUX FHUDPLFL SRU(aR D V H SFRXU RD]FLHWHDDW܈HL USHROUDRW]LLYWăD W HvQ IRVW UHSUH]HQWDWH FRPSDUDWLY LPDJLQLOH SRODUL VLPXOHD]ă H[SHULPHQWXO GH PăVXUDWRUL SLH]RHOHF
(a) (b) (c)
Fig. 3 6WUXFWXUL GH GRPHQLL GHWHUPLQDWH OD VDWXUDа SRUR]LWDWH UHODWLYă vQ FD]XO vQ FDUH FRQILJX D[D OXQJă SDUDOHOă O X QFJ ă FSXH USSRHUQLG LDFOXOQDJULăа LS HF XG L
6H REVăHVUDYWăX UDF܊LD FRPSOHWă VH UHDOL]HD]ă vQ H܈DQWL±FRXQOXRODXULH D JDOEHQă DSURDSH SHVWH WRW SUDF cktevD ]RQH PLFL vQ -YDH FOLXQQDJWXDOW HGDL USHRFU܊LOHRLU F kGPHSXOXL FkQG FkPSXO HVWH DSOLFDW SDUDOHO FX D[D OXQJă GH DVHPHQHD GHIRUPODXULH D FUDHUOHD WVLHY ăR EDV HU܈YDăQ W܈LLR QvXQ ) GHWHUPLa Q D W ă G H6 LVWHPXO L]RWURS FX SRUL VIHULFL H[WLQVă vQVă H[LVWă FHYD PDL PXOW Hv QU HFJDL]XXQOL SFU
SRODUL]D܊LD WRWDOă YD IL PDLa P L F ă ܈'LD FGăH SDRVUHLPLH Q OXQJă SHUSHQGLFXODUă SH GLUHF܊LD FkPSXOXL DSOL
OD VDWX U D ܊FL H D)YLkJQG ]RQH H[WLQVH FX RULHQWăUL FD] SRODUL]D܊LD WRWDOă YD IL ܈a0L.5% . PDL PLFă ܈L G
Porous ceramics
r.d. 78%
Isotropic Parallel Perpendicular
0,8
0,6
Polarization (a.u.)
0,4
0,2
0,0
-0,2
-0,4
-0,6
-0,8
-15
-10 -5 0
5 10 15
0,25
Porous ceramics
Isotropic
Parallel
r.d. 78%
Perpendicular
Permittivity (a.u.)
0,20
0,15
0,10
0,05
0,00
-12 -9 -6 -3 0 3 6 9 12
Electric field (a.u.)
Electric field (a.u.)
)LJ &LFOXUL GH KLVHW H(U H ]FLDVO F3X O(D W HЮ LG LWQX QVDLEPLXOOL FHUDPLFL SRURDVH FX DFHHDЮL GHQVLWDWH SRU L]RWURSă E FX SSRRUULL DDOOXXQQJJLLааLL SSDHUUDSOHQOGLL F X OFD U
)LJ SUH]LQWă FLFOXUP(EL) O܈HL DHO HK LWVXHWQሺܧHDሻ,UEcaHLlc]uOlaLteVWdi năD܊OLHL VLPXOăUL 0RQWH &DUOR vQ FHOH WUHL FD]XUL 3RO SDUDOHOH E LDU FHOH PDL PLFL FRUHVSXQ-VGH FvRQQWI
DFHVWH GRXă GOHLVPFLUWHHV F ă3WHR DH]UሺܧRHሻ,Q tuDDna b ilGitaHteaS݊HሺܧQሻൌGHHሺͲQሻȀ܊HሺHܧሻLD UH DFHO WUHQG GH H[HPSOX SHQWUX XQ Fka P S H O HFRWQUILFaJ 0.X7G8UHD ܊ L
(Fig. 3a) ܈i respectiv a0.64 (Fig. 3c).
Proiectare de microstructuri ceramice piezo-/piroelectrice, folosind modele teoretice, cu FOM vPEXQăWăаLWH 0RGHO )(0 аa'd e pSorHozQitaWte Ua pXer miDtiv ităGiаiHizWotrHopUe PLQD
ÌQWUXFkW DWkW vQ DSOLFD܊LLOH SLt U(FROMH)OesHteFinWveUrs LFH SURSRU܊LRQDOă FX SHUPLWLYLWDWHD PHGLXOXL VH L ULGLFDW UăVSXQVXO SLUR SLH]RHOHFWULF DO VLVWHP VLVWHP U$D܈WDă F܈XLP PDRGHOXO ' -DS UGHH]PHRQQWVDWU DWQ WDHQUWLHRUL
grupului [6@ QX GRDU FDQWLWDWHD GH SRUL FRQFHQWUD GHIRUPDUHD UHODWXLQYăDE L SOHLUWPDLWWHLDY L WFDLW ܈HLD G܈LV WULEX܊L FkPSXOXL DSOLFDW
$VWIHO vQ FDGUXO DFHVWXL RELHFWLY VH YRU
DGHFYDWă D SHUPăLnWu ILLYHL WăG܊HLWLU L PsuHGluQDi pWUiroD - OFSăDL UHUH]ă RVHSOXHQFWULF PD[LPL]H]H )20 vQ YHGHUHD DSOLFăULL DFHVWRUD
VLPXOăUL IROemReVntuLluQi fGini t (PFEHMW) [R7]GcDare vHor Opermite proiectarea de microstructuri favorabilH vQ VFRXXX XD[LPL]ăULL )20
ÌQ SULPD SDUWH D DFHVWXL RELHFWLY D IRVW G GHSHQGHQ܊D SHUPLWLYLWă܊LL vQ IXQF܊LH GH SRUR]L
electrice ale sistemului VXQW RE܊LQXWH SULQ UH]ROYDUHD HFXD܊LH
ήሺHMሻൌͲ, (7)
unde MHVWH SRWHQ܊LDOH XSOH UHPOLHWFLWYULLWFD WOHRDF DOOR F DLODăU D PHGLX a LDU vQ LQWHULRRUVXWO JSHRQUHLUODR܊UL DHOVHWDHW R U v3QR UVLV FRUHVSXQ]ăWRDUH FRQIL-JSXDUD܊OLHHOL G)HL J F RQ GDH Q V DSWHR UD O
GLIHUHQ܊ă GH SRWHQ܊LDO kmFpuRl QeleGctrLic܊esLteLo rienOtaDt p erpOenLdiPcuLlarWpDe 'L
HOHFWUR]L ܈L WDQJHQ܊LDO aO1DH XVPXDSQUQD I H ܊6HLOVHW HOPDXWOH UDD OI WHWUDHGULFH LDU SRWHQ܊LDOXO vQ LQWHULRUXO IL
corespunzăWRDUH QRGXULORU
MሺݔǡݕǡݖሻൌMMM , (8)
ଵ ଵ ଶ ଶ
ଷ ଵଷ
vQ eFUDHUSHU H]LQWă QXPăUXO VHXOQHWP HIQXWQXFO܊XLL OFMHRV QXGVQHLW G LHSQURWDWHWHU QS
ORFDOH vQ FHOH SDWUX QR݇GൌXͳǡUʹǡL͵) D)ORHO RHVOLHQPGH QWSUXROXFLH GXF FDOFXOH DOJHEULFH PDWULFLDOH FX FRQGL܊LL OD OL GLQ UH܊HDXD GH GLVFUHWL]DUH &XQRVFkQG SRWHQ܊L
ܧԦൌെ݃ݎܽ ܸ݀
(9)
/D SDVXO XOWHULRU VH GHWHUPLQD HQHUJLD HOHFWU WXWXURU HOHPHQWHORU ܈L DFHDVWD VH FRQVLGHUă HJ
echivalent de volum ݒ௧ FăU-DX LDS OL FVDܧW ܈XLQ DFYkkPQSG SHUPHLW:LYLWDWHD
ܹ ൌଵσே Hܧଶݒ ൌ ଵܧଶ ݒ, (10)
௧௧ଶ ୀଵ ଶ ௧
vQ NFHDVUWHH QXPăUXO WHRǡWܧDǡݒO VGXHQ WH OSHPUHPQLWHL YLDWUD WHD ORFD
volumul elementului ݇considerat.
(a) (b)
(c) (d)
)LJ D 6LVWHPXO SRURV FRQVLGHUDW vQ VLPXO FkPSXO ORFDOV FUDHOSDU HG]HH QFWXDOWR UvLQ G 'HSHQGHQаD G
5H]XOWDWHOH FDOFXOHORU FX )(0 VXQW SUH]HQWD
F VXQW UHSUH]HQWDWH văGQH VSFRDWOHDQ ܊GOLHLD FODX WOGăHR U V LL9 V WDSHSHPQXWO
grosimea de 1mm.
3HQWUX D GHWHUPLQDi HGIHSFHWQLGYHHQ ܊FDD SIHXUQPFL܊WLHY LGWHă ܊ XUPăWRULL SD܈L DX IRVW JHQHUDWH PLFURVWUXFWXU
fiecare caz, s-D XUPDW SURFHGXUD GHVFULVă DQWHU-aLdReteUrm in at $VW SHUPLWLYLWDWHD HIHFWLYă ܈L D IRVW UHSUH]HQWDWă
Rezultat DO D܊Fii WAIL.1 YestLe WGăH]YROWDUHD GH PRGHOH FDRpPenEtruLQDW
a monitoriza HYROX܊eLniiDlor feGroRelPectrice ܈i estimarea GHSODorVfiăecUăruLi Onod dintr-o UH܊HD
discretizaWăpentru a evalua la fiecare pas deformarea unui sistem feroelectric dens, vQ PDL PX VLWXvDQ܊ LDLE V WHQ܊D FkPS, XvOQX LW LHPOSHXFOW UGLHFV FHU[LWHHUULQL ܈FLvXQU EH
timpul parcurgerii ciclurilor de histerezis sub ckPSXേ۳O. 3 URFHGXUD GH]YROWsDe Wă
a fRVW IRORVLWă ܈L SHQWUXi te aFleHpUoriDlorP(iLzoFtroLpi - VSIRHUURaDLniVFzoHLtro pi F܈±XL I DOXQ), JiarLr܊ezLultatele reprezentate comparativ au arăWDWS RFOăD UL]D܊LD ܈L GHIR
UăVSXQVXO vSQL H]PRDHWcOHerHaUmFLicWeDUpOoLrHoFa s e d epind de forma porixxx ܈L GH GLUH
ckPSXOXL apHlicOatH. UFn WaltUreLzuFlta t DO DFOWRLUY LWQăW܊ULHSULQfoVloHsin dDV LIPRXVOWă UFL
0RQWH &DUOR DX IRVW FDOFXOPD(EW) H S܈ULH FUXHPS U܈HL]H ሺ۳HሻWQvXWQQD DWEH
materiale poroase cu diferite forme ale porilor -܈DL DVUăWDW LPSDFWla XdifOeri teFvaklorPi SXO ale acestuia (AI.2). ÌQ FRQWenLtruQpXroDiecUtaHrea d e mSicrostructuri ceramice piezo-/piroelectrice s-a
utilizat modelul FEM 3D, iar rezultatul RE܊LdinQFXDWOFXVOLHPOrXHileO dăe܈mLicrostructuri realistice
DX DUFă DRW SRUR]LWDWH UHODWLYă D FHUDPLFLL GH FHUDPLFLL GHQVH OD LDU SHQWUX R SRUR]LWDW
ID܊ă GH FHD FRUHVS.X(AQI.]3 văa cWonRtinDuaUvHQ P D. W H U LDOXOXL G Rezultatele RE܊LQvXQW HFDGUXO , sDtudFiuHl HVIWHFLW XHOWXDLSas HuSSURDU RS]ULRWSăU܊L
IXQF܊aLleRmQateDriaOlelHor ceramice de BaTiO3 au IăFXW VunXeiEluLcrHăFUWLX O܈ WLLQ܊LvnILFH
JOURNAL OF ALLOYS AND COMPOUNDS ܈L GLVHacPesLtorQa DvUQH DF Da G U XFOR QIHUL
LQWHUQ.DÌ܊QL RHQWDUDOPSHăHWOaRcHeDs teUXstHud ii vor continua, iar rezultatele teoretice vor fi comparate cu
datele experimentale RE܊LQXWH SH FHUDPoiLecFtulLui. SURGXVH vQ FDGUXO