• Title/Summary/Keyword: $L_C$-property

Search Result 459, Processing Time 0.029 seconds

Fabrication and Characterization of $TiB_2$-based Cermet Using SUS316L Metal Binder (SUS316L결합상을 이용한 $TiB_2$ 서멧합금의 제조와 특성평가)

  • An, Dong-Gil
    • Korean Journal of Materials Research
    • /
    • v.10 no.12
    • /
    • pp.838-844
    • /
    • 2000
  • For the fabrication of titanium diboride($TiB_2$)- based cermet as applications of cutting tools and wear resistant materials, a binder metal with good mechanical properties and sinterability is essential. In this study, SUS316L was chosen for the binder metal to obtain a new $TiB_2$ cermet with superior hardness and toughness.$TiB_2$-SUS316L cermets were densified to relative density of more than 99% by pressureless sintering at temperature above $1650^{\circ}C$ The flexural strength was up to 1290MPa at 10vo1%SUS316L cermet in spite of the formation of $Fe_2$B phase during the sintering. The fracture toughness was obtained up to $6MPam^{1/2}$ with Victors hardness over 18Gpa. These hardness and fracture toughness combinations are better than those of conventional cermet. The high temperature strength remarkably decreased by the plastic deformations of SUS316L binder phase at nearby $800^{\circ}C$ .

  • PDF

Synthesis and Charaterization of Photoluminescent and Electrochemical Property for Diruthenium Complex with Diimine Bridge (디이민 가교제를 갖는 이핵 루테늄 착체의 광발광 및 전기화학적 특성)

  • Kim, Dong-Hwan;Kim, Hwa-Seon;Kwak, Ji-Hoon;Lee, Jee-Hoon;An, Ho-Guen;Woo, Myung-Woo;Ruimao, Hua;Jung, Min-Chul
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 2006.11a
    • /
    • pp.296-297
    • /
    • 2006
  • 유기EL의 발광재료로 쓰일 수 있는 이핵 루테늄착체는 $Ru(bpy)_2Cl_2$와 새롭게 디자인한 가교체 (Bis(-2,2'-dipyridyl ketenylidene)-N,N-1,6-diphenylene diamine)의 반응으로부터 합성하였고, FT-IR, $^1H$-NMR, $^{13}C$-NMR, UV-vis, P.L, C.V를 이용하여 착체의 구조분석, 광학적 특성과 전기화학적인 특성을 측정하였다.

  • PDF

LOCAL SPECTRAL PROPERTIES OF SEMI-SHIFTS

  • Yoo, Jong-Kwang;Kim, Yong-Il
    • Journal of applied mathematics & informatics
    • /
    • v.28 no.1_2
    • /
    • pp.499-507
    • /
    • 2010
  • In this note, we study the local spectral properties of semi-shifts. If $T\;{\in}\;L(X)$ is a semi-shift on a complex Banach space X, then T is admissible. We also prove that if $T\;{\in}\;L(X)$ is subadmissible, then $X_T(F)\;=\;E_T(F)$ for all closed $F\;{\subseteq}\;\mathbb{C}$. In particular, every subscalar operator on a Banach space is admissible.

Influence of Hot-Extrusion on Mechanical Properties of AZ31B Magnesium Alloy Sheet (AZ31B 마그네슘 합금의 기계적 특성에 미치는 열간압출의 영향)

  • Kim Yong-Gil;Choi Hak-Kyu;Kang Min-Cheol;Jeong Hae-Yong;Bae Cha-Hurn
    • Korean Journal of Materials Research
    • /
    • v.15 no.1
    • /
    • pp.25-30
    • /
    • 2005
  • The microstructural changes by hot extrusion of AZ31B magnesium alloy were observed, and the relation to the tensile property was examined. The tensile properties as oriented longitudinal(L), half transverse(HT) and long transverse(LT) to the extrusion direction were investigated at $20^{\circ}C,\;100^{\circ}C,\;200^{\circ}C,\;300^{\circ}C\;and\;400^{\circ}C$, respectively. As the results, many recrystallized small grains distributed uniformly in large banded microstructures formed along the extrusion direction. The grain size of as-extruded specimen was around $30\~150\;{\mu}m$. As increasing the test temperature the tensile and yield strength with respect to the angle between the axis of the tensile and the longitudinal direction in extrusion was decreased, but their elongation were increased and their deviation between L and LT specimens have disappeared from $300^{\circ}C$. This mechanical anisotropy was reduced at elevated temperatures and almost disappeared at $400^{\circ}C$. It was considered that the homogenization was occured by the recrystallization and the change of slip system was occurred during tensile test process in elevated temperatures.

A Two-Dimensional Terrace-Like N-heterocyclic-Pb(II) Coordination Compound: Structure and Photoluminescence Property

  • Ma, Kui-Rong;Zhu, Yu-Lan;Zhang, Yu;Li, Rong-Qing;Cao, Li
    • Bulletin of the Korean Chemical Society
    • /
    • v.32 no.3
    • /
    • pp.894-898
    • /
    • 2011
  • The first example of lead compound from $Pb(NO_3)_2$ and $H_3L$ N-heterocyclic ligand $(H_3L\;=\;(HO_2C)_2(C_3N_2)(C_3H_7)CH_2(C_6H_4)(C_6H_3)CO_2H)$, $[Pb_4(L')_4]{\cdot}5H_2O$ 1 (L' = OOC$(C_3H_7)(C_3N_2)CH_2(C_6H_4)(C_6H_3)COO)$, has been obtained under hydrothermal condition by decarboxylation, and characterized by elemental analysis, IR, TGDTA, and single-crystal X-ray diffraction. Compound 1 possesses a rare two-dimensional upper-lower offset terrace-like layer structure. In 1, crystallographic distinct Pb(II) ion adopts five-coordination geometry, and two lattice water molecules occupy the voids between 2-D layers. Results of solid state fluorescence measurement indicate that the emission band 458 nm may be assigned to $\pi^*-n$ and $\pi^*-\pi$ electronic transitions within the aromatic systems of the ligand L', however, the emission bands centred at 555 nm, 600 nm and 719 nm may be derived from phosphorescent emission ($\lambda_{excitation}$ = 390 nm).

THE RELATION PROPERTY BETWEEN THE DIVISOR FUNCTION AND INFINITE PRODUCT SUMS

  • Kim, Aeran
    • Honam Mathematical Journal
    • /
    • v.38 no.3
    • /
    • pp.507-552
    • /
    • 2016
  • For a complex number q and a divisor function ${\sigma}_1(n)$ we define $$C(q):=q{\prod_{n=1}^{\infty}}(1-q^n)^{16}(1-q^{2n})^4,\\D(q):=q^2{\prod_{n=1}^{\infty}}(1-q^n)^8(1-q^{2n})^4(1-q^{4n})^8,\\L(q):=1-24{\sum_{n=1}^{\infty}}{\sigma}_1(n)q^n$$ moreover we obtain the number of representations of $n{\in}{\mathbb{N}}$ as sum of 24 squares, which are possible for us to deduce $L(q^4)C(q)$ and $L(q^4)D(q)$.

EEG model by statistical mechanics of neocortical interaction

  • Park, J.M.;Whang, M.C.;Bae, B.H.;Kim, S.Y.;Kim, C.J.
    • Journal of the Ergonomics Society of Korea
    • /
    • v.16 no.2
    • /
    • pp.15-27
    • /
    • 1997
  • Brain potential is described using the mesocolumnar activity defined by averaged firings of excitatory and inhibitory neuron of neocortex. Lagrangian is constructed based on SMNI(Statistical Mechanics of Neocortical Interaction) and then Euler Lagrange equation is obtained. Excitatory neuron firing is assumed to be amplitude- modulated dominantly by the sum of two modes of frequency .omega. and 2 .omega. . Time series of this neuron firing is calculated numerically by Euler Lagrangian equation. I .omega. L related to low frequency distribution of power spectrum, I .omega. H hight frequency, and Sd(standard deviation) were introduced for the effective extraction of the dynamic property in the simulated brain potential. The relative behavior of I .omega. L, I .omega. H, and Sd was found by parameters .epsilon. and .gamma. related to nonlinearity and harmonics respectively. Experimental I .omega L, I .omega. H, and Sd were obtained from EEG of human in rest state and of canine in deep sleep state and were compared with theoretical ones.

  • PDF

Reduced-order $H_{\infty}$ controller Design of Drum-type boiler system (드럼형 보일러 시스템의 저차 $H_{\infty}$ 제어기 설계)

  • Choi, S.C.;Jo, C.H.;Seo, Jin.H.
    • Proceedings of the KIEE Conference
    • /
    • 1994.11a
    • /
    • pp.366-369
    • /
    • 1994
  • In this paper, reduced-order $H_{\infty}$ robust controller is designed for the drum-type boiler system. From the known nonlinear dynamic model, a linearized multivariable model is obtained. To reduce order of robust controller, observer-based proper $H_{\infty}$ compensator is designed. The designed controller has robust property against the influence of sensor noise, system parameter variation and model uncertainty. A good Performance of the designed controller is shown by simulation.

  • PDF

3-Dimensional Tunnel Analyses for the Prediction of Fault Zones (파쇄대 예측을 위한 터널의 3차원 수치해석)

  • 이인모;김돈희;이석원;박영진;안형준
    • Journal of the Korean Geotechnical Society
    • /
    • v.15 no.4
    • /
    • pp.99-112
    • /
    • 1999
  • When there exists a fault zone ahead of the tunnel face and a tunnel is excavated without perceiving its existence, it will cause stress concentration in the region between the tunnel face and the fault zone because of the influence of the fault zone on the arching phenomena. Because the underground structure has many unreliable factors in the design stage, the prediction of a fault zone ahead of the tunnel face by monitoring plans during tunnel construction and the rapid establishment of appropriate support system are required for more economical and safer tunnel construction. Recent study shows that longitudinal displacement changes during excavation due to the change of rock property, and if longitudinal displacement and settlement, which are measured in the field, are considered together in displacement analysis, the prediction of change in rock mass property is possible. This study provided the method for the prediction of fault zones by analyzing the changes of L/C and (Ll-Lr)/C ratio (L= longitudinal displacement at crown, C = settlement at crown, Ll = longitudinal displacement at left sidewall, Lr = longitudinal displacement at right sidewall) and the stereographic projection of displacement vectors which were obtained from the 3-D numerical analysis of hybrid method in various initial stress conditions.

  • PDF