• 제목/요약/키워드: $D_{r}(D_2G)$

검색결과 2,385건 처리시간 0.034초

후산정체 젖소에 있어서 Lipopolysaccharide의 처리가 자궁 회복에 미치는 영향 (Effect of Lipopolysaccharides Treatment on Uterine Involution in Dairy Cows with Retained Placenta)

  • 백광수;박성재;박수봉;이왕식;김현섭;정경용;기광석;서국현;전병순;안병석;김태일
    • 한국수정란이식학회지
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    • 제21권3호
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    • pp.233-239
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    • 2006
  • 본 연구는 후산정체 젖소에 있어서 Lipopolysaccharide의 처리가 자궁 회복에 미치는 영향을 조사하기 위하여 2004년부터 2005년까지 2년간에 걸쳐 축산연구소와 전문 경영체 농장에서 사육중인 홀스타인 착유우 중 분만 후 12시간이 경과하여도 태반이 배출되지 않았던 후산정체우 33두를 대상으로 LPS $100{\mu}g$구, LPS $200{\mu}g$구 및 대조구 각각 11두씩을 공시하였으며 분만 후 20일째에 대조구는 PBS를, 처치구는 LPS를 자궁내에 주입하여 분만 후 40일째에 초음파 측정을 통하여 자궁의 크기 및 자궁내 삼출물의 저류 정도를 조사하여 다음과 같은 결과를 얻었다. 1.자궁각의 크기에 있어서 30 mm이하인 경우는 대조구 45.5%, LPS $100{\mu}g$구 100%, LPS $200{\mu}g$구 72.7%였고 $31{\sim}50mm$인 경우는 대조구 27.3%, LPS $100{\mu}g$구 0%, LPS $100{\mu}g$구 18.2%였으며 51 mm이상인 경우는 대조구 27.3%, LPS $100{\mu}g$구 0%, LPS $200{\mu}g$구 9.1%였다. 2. 삼출액의 저류 상태에 있어서 삼출액이 거의 없는 경우는 대조구 18.2%, LPS $100{\mu}g$구63.6%, LPS $200{\mu}g$구 54.6%였고 자궁강내에 삼출액이 소량 있는 경우는 대조구 36.4%, LPS $100{\mu}g$구 36.4%, LPS $200{\mu}g$구 36.4%였으며 자궁강내에 삼출액이 고여 있는 경우는 대조구 45.5%, LPS $100{\mu}g$구 0%, LPS $200{\mu}g$구 9.1%였다.

New Cu Process and Short Channel TFT

  • Yang, J.Y.;Hong, G.S.;Kim, K.;Bang, J.H.;Ryu, W.S.;Kim, J.O.;Kang, Y.K.;Yang, M.S.;Kang, I.B.;Chung, I.J.
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2009년도 9th International Meeting on Information Display
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    • pp.1189-1192
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    • 2009
  • Short channel a-Si:H TFT devices with Cu electrodes have been investigated. Short channel TFTs are defined by new plasma etch process. When the channel length becomes shorter, the TFT characteristics (threshold voltage, off current, sub threshold voltage, etc.,) are degraded. These degraded characteristics can be improved through the hydrogen plasma treatment and new gate insulator structure. Using these processes, 15.0 inch XGA LCD panel was fabricated successfully where the channel length of the TFT devices was about 2.5 micrometers.

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THE STABILITY OF PEXIDERIZED COSINE FUNCTIONAL EQUATIONS

  • Kim, Gwang Hui
    • Korean Journal of Mathematics
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    • 제16권1호
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    • pp.103-114
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    • 2008
  • In this paper, we investigate the superstability problem for the pexiderized cosine functional equations f(x+y) +f(x−y) = 2g(x)h(y), f(x + y) + g(x − y) = 2f(x)g(y), f(x + y) + g(x − y) = 2g(x)f(y). Consequently, we have generalized the results of stability for the cosine($d^{\prime}Alembert$) and the Wilson functional equations by J. Baker, $P.\;G{\check{a}}vruta$, R. Badora and R. Ger, and G.H. Kim.

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X-선에 대한 마우스의 내력 (Studies on Tolerance of Mice to X-rays)

  • 김정진
    • 한국동물학회지
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    • 제6권2호
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    • pp.11-15
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    • 1963
  • A total of 220 adult male mice (18-20g) of the S.M. strain were divided into ten experimental and control groups. The total-body X-ray irradiation doses used were 50 r, 100r, 200r, 400r, 600r, 800r, 1,000r, 1,200r, 1,400r, and1,600r. The respiratory arrest (mortality) caused by each irradiation doses were observed for 30 days. Relationships between irradiation doses and survival time and percentage of response were examined. From this experiment, a formula was obtained to express the relationship among three factors, which may be presented as follows : {{{{{{{{P= { 10} over { SQRT { 2 pi } } INT _{ - INF }^{ p'} e-{(p'-50)^2 } over {200 }dp···(a) p'=100 LEFT { t^0.3- LEFT ( { { 16.9965} over {D-60 } } RIGHT ) ^{ { 1} over {2.5 } } } / LEFT { LEFT ( { 26372.43} over {D-81.86 } RIGHT ) ^{ { 1} over {2.5 } } -( { { 16.9965} over {D-60 } } RIGHT ) ^{ { 1} over {2.5 } } ···(b) p= { (D-60) t^0.75-16.9965} over {0.2186 t^0.75 +263.55434 }····(c) }} {{{{P= { 10} over { SQRT { 2 pi } } INT _{ - INF }^{ p'} e-{(p'-50)^2 } over {200 }dp···(a) p'=100 LEFT { t^0.3- LEFT ( { { 16.9965} over {D-60 } } RIGHT ) ^{ { 1} over {2.5 } } } / LEFT { LEFT ( { 26372.43} over {D-81.86 } RIGHT ) ^{ { 1} over {2.5 } } -( { { 16.9965} over {D-60 } } RIGHT ) ^{ { 1} over {2.5 } } ···(b) p= { (D-60) t^0.75-16.9965} over {0.2186 t^0.75 +263.55434 }····(c)

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NUMERICAL METHODS FOR SOME NONLINEAR STOCHASTIC DIFFERENTIAL EQUATIONS

  • El-Borai, Mahmoud M.;El-Nadi, Khairia El-Said;Mostafa, Osama L.;Ahmed, Hamdy M.
    • Journal of the Korean Society for Industrial and Applied Mathematics
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    • 제9권1호
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    • pp.79-90
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    • 2005
  • In this paper we study the numerical solutions of the stochastic differential equations of the form $$du(x,\;t)=f(x,\;t,\;u)dt\;+\;g(x,\;t,\;u)dW(t)\;+\;\sum\limits_{|q|\leq2m}\;A_q(x,\;t)D^qu(x,\;t)dt$$ where $0\;{\leq}\;t\;{\leq}\;T,\;x\;{\in}\;R^{\nu}$, ($R^{nu}$ is the $\nu$-dimensional Euclidean space). Here $u\;{\in}\;R^n$, W(t) is an n-dimensional Brownian motion, $$f\;:\;R^{n+\nu+1}\;{\rightarrow}\;R^n,\;g\;:\;R^{n+\nu+1}\;{\rightarrow}\;R^{n{\times}n},$$, and $$A_q\;:\;R^{\nu}\;{\times}\;[0,\;T]\;{\rightarrow}\;R^{n{\times}n}$$ where ($A_q,\;|\;q\;|{\leq}\;2m$) is a family of square matrices whose elements are sufficiently smooth functions on $R^{\nu}\;{\times}\;[0,\;T]\;and\;D^q\;=\;D^{q_1}_1_{\ldots}_{\ldots}D^{q_{\nu}}_{\nu},\;D_i\;=\;{\frac{\partial}{\partial_{x_i}}}$.

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Sparkover Voltage Estimation of Standard Sphere Gaps for Negative Polarity by Calculation of Ionization Index

  • Nishikori, Yasuo;Kojima, Soji;Kouno, Teruya
    • KIEE International Transactions on Electrophysics and Applications
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    • 제4C권2호
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    • pp.45-50
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    • 2004
  • The field utilization factor (equation omitted) (the mean electric field / the maximum electric field) of standard sphere gaps was calculated by the charge simulation method, taking into account the ground plane and shanks. n changes mainly with g/r and slightly with 1$_1$, 1$_2$ and 1, where D=2r is the sphere diameter, g is the gap length, 1$_1$ and 1$_2$, respectively, are the lengths of the upper and lower shank, and t is the shank diameter. Generally, (equation omitted) increases as 1$_1$,1$_2$ and t each becomes larger. IEC standard 60052(2002) limits t$\leq$0.2D 1$_1$$\geq$1D and prescribes A=1$_2$+D+g where A is the height of the spark point on the upper sphere. Therefore, (equation omitted) is the largest when A=9D and the smallest when A=3D. The simple equation of a straight line, (equation omitted)=1- (g/3r), can generally be used as a representative value of (equation omitted) for a wide variety of sphere diameters that are permitted by the IEC standard. The maximum electric field E$_{m}$ at sparkover of standard air gaps has also been calculated by the relation E$_{m}$=V/(equation omitted)g). E$_{m}$ describes a U-curve for g/r, up to the sphere diameter of 1 m. Moreover, for 1.5-m and 2-m diameters and especially .for negative polarity, sparkover voltages have been calculated by integration of the ionization index.index.

중생 흑자색 찰벼 신품종 '보석흑찰' (A New Black Pericarp, Medium-Ripening Glutinous Rice Cultivar 'Boseogheugchal')

  • 이점호;이상복;김홍열;양창인;김명기;전용희;이규성;김연규;정오영;황흥구;최용환;양세준;조영찬;오세관;예종두;이정희;원용재;이정일;정국현;황기호
    • 한국육종학회지
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    • 제43권6호
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    • pp.600-605
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    • 2011
  • 보석흑찰(수원512호)은 생리활성기능을 가지고 있는 안토시안 함량이 높고 중생이며 흑자색 찰벼 품종을 개발하고자 유색찰 우량계통 SR18638-B-B-B-18-2와 흑자색 유색미 유전자원 흑미 H31을 교배하여 계통육종법으로 육성한 신품종이다. 선발된 우량계통에 대해 2005년부터 2006년까지 2년간 생산력 검정시험을 수행한 결과, 중생이고 색소의 착색과 수량성이 양호한 SR24098-17-2-2-3-2-2 계통을 선발하여 '수원512호'로 계통명을 부여하였다. '수원512호'는 2006-2008년 3년간 지역적응시험에서도 그 우수성이 인정되어 2008년 12월 농촌진흥청 농작물 직무육성 신품종선정위원회에서 국가품종목록에 등재할 것을 결정하고 '보석흑찰'로 명명하였다. 1. 출수기는 중부 평야지에서 8월 17일로 조생종 '흑진주'에 비해 24일 늦은 중만생종이다. 벼키는 85 cm로 '흑진주'보다 큰 편이며, 포기당 이삭수는 12개로 흑진주와 거의 비슷하고, 이삭당 벼알수는 94개로 '흑진주'에 비해 약간 많다. 현미천립중은 21.6 g으로 '흑진주'에 비해 다소 무겁다. 2. 도열병, 흰잎마름병, 바이러스병 및 멸구류에 대한 저항성이 없으며, 포장도복에 강하고 50일묘 늦심기에서 불시출수와 위조현상이 나타나지 않았으며, 성숙기에 하엽 노화의 진행이 늦었다. 냉수처리구에서 임실율이 54%로 중도 내냉성을 보인다. 수발아율은 1.3%로 거의 되지 않았으며, 도복에 강하다. 3. 현미종피는 진한 흑자색이며 배유는 찰성이다. 안토시아닌(C3G) 함량은 717 mg/1000 g 으로 '흑진주벼' 보다 1.6배 높으며, 단백질함량은 6.4%로 '흑진주' 보다 낮았으며 정현비율은 79.5%로 '흑진주'와 비슷하다. 4. '보석흑찰'의 평균 현미수량은 보통기 보비재배에서 4.82 MT/ha으로 '흑진주' 대비 19% 증수되었다.

GENERALIZED DERIVATIONS WITH CENTRALIZING CONDITIONS IN PRIME RINGS

  • Das, Priyadwip;Dhara, Basudeb;Kar, Sukhendu
    • 대한수학회논문집
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    • 제34권1호
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    • pp.83-93
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    • 2019
  • Let R be a noncommutative prime ring of characteristic different from 2, U the Utumi quotient ring of R, C the extended centroid of R and f($x_1,{\ldots},x_n$) a noncentral multilinear polynomial over C in n noncommuting variables. Denote by f(R) the set of all the evaluations of f($x_1,{\ldots},x_n$) on R. If d is a nonzero derivation of R and G a nonzero generalized derivation of R such that $$d(G(u)u){\in}Z(R)$$ for all $u{\in}f(R)$, then $f(x_1,{\ldots},x_n)^2$ is central-valued on R and there exists $b{\in}U$ such that G(x) = bx for all $x{\in}R$ with $d(b){\in}C$. As an application of this result, we investigate the commutator $[F(u)u,G(v)v]{\in}Z(R)$ for all $u,v{\in}f(R)$, where F and G are two nonzero generalized derivations of R.

연 노출 근로자들의 혈장 δ - aminolevulinic acid 량과 연 노출 지표들과의 관련성 (The Relationships between Plasma δ - aminolevulinic acid Concentration and Lead Exposure Indices in Lead Workers)

  • 김진호;안규동;이성수;황규윤;김용배;이병국
    • 한국산업보건학회지
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    • 제10권2호
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    • pp.165-172
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    • 2000
  • This study was carried out to investigate relationship between plasma $\delta$ - aminolevulinic acid (ALAP) and lead exposure indices in exposure to lead. The subjects were 218 male workers in 2 storage battery companies and 2 secondary smelting companies. Blood lead(PbB), blood zinc-protoporphyrin( ZPP), urinary $\delta$ - aminolevulinic acid (ALAU), hemoglobin(Hb), and hematocrit(Hct) were measured as lead exposure indices. The results were as follows, 1. The means of blood lead and blood ZPP concentration of subjects were $27.2{\pm}14.0{\mu}g/d{\ell}$ and $55.1{\pm}47.6{\mu}g/d{\ell}$, respectively. The means of plasma $\delta$ - ALA and urinary $\delta$ - ALA concentration were $18.9{\pm}25.1{\mu}g/d{\ell}$ and $2.1{\pm}4.6mg/{\ell}$, respectively. 2. The concentration of ALAP was $11.2{\mu}g/{\ell}$ for below $20{\mu}g/d{\ell}$ PbB, $12.8{\mu}g/{\ell}$ for from $21-40{\mu}g/d{\ell}$ PbB, and $51.2{\mu}g/{\ell}$ for over $40{\mu}g/d{\ell}$ PbB, respectively. 3. ALAP was significantly correlated with ALAU(r=0.829, p<0.01), ZPP(r=0.724, p<0.01) and PbB(r=0.552, p<0.01).

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PREPARATION AND PROPERTIES OF OIL-BASED MAGNETIC FLUIDS WITH THE SYNTHESIZED MAGNETITE

  • Jang, K.O.;Doh, S.W.;Cho, S.I.;Shon, H.J.;Hur, W.D.
    • 한국자기학회지
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    • 제5권5호
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    • pp.819-823
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    • 1995
  • The oil-based magnetic fluids were sysnthesized using ultra-fine $Fe_{3}O_{4}$ powder dispersed in hydrocarbon oil. To synthesize ultra-fine $Fe_{3}O_{4}$, we carried out the experiments varying the pH of reacting medium and the initial concentration of $Fe^{2+}$. We also investigated the amount of oleic acid to obtain a stable dispersion and the proper base oil of MF for loudspeaker application. The limits of adsorbed amount of oleic acid on the $Fe_{3}O_{4}$ surface were approximately 35~40 percents of the total magnetite weight. As the $Fe_{3}O_{4}$ content increased from 0.1g/cc to 0.6g/cc, the viscosity of oil-based magnetic fluid increased from 1,063cP to 1,828cP, and its saturation magnetization at 10kOe increased from 66G to 242G. When we tested the MF sample to a commercial speaker, improvements were noted.

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