• 제목/요약/키워드: ND2

검색결과 8,722건 처리시간 0.034초

파장가변 티타늄 사파이어 레이저로 펌핑하는 연속발진 Nd:YVO4/KTP 레이저의 출력 특성 (Output power characteristics of a CW Nd:YVO4/KTP laser pumped by a tunable Ti:Sapphire laser)

  • 추한태;안범수;김규욱;이치원
    • 한국광학회지
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    • 제13권2호
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    • pp.140-145
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    • 2002
  • 선폭 0.2nm인 파장가변 티타늄 사파이어 레이저를 펌핑 레이저로 사용하여 펌핑 레이저의 5편광(E┴$\pi$)과 P-편광(E∥$\pi$) 그리고 파장 변화 등에 따라 두께 1 mm인 Nd:YVO$_4$결정의 흡수율 및 연속 발진 Nd:YVO$_4$/KTP 레이저의 출력 특성을 측정하였다. 그 결과 S-편광 및 P-편광 펌핑 레이저의 파장에 따른 Nd:YVO$_4$결정의 최대 흡수율은 각각 809.4 nm일 때 82% 및 808.8 nm일 때 98%로 측정되었으며, 기본파인 Nd:YVO$_4$레이저(1064 nm) 출력의 기울기 효율은 각각 43% 및 52%로 측정되어 1000 mW 출력의 P-편광 펌핑 레이저에 대하여 최대 516 mW의 Nd:YVO$_4$레이저 출력을 얻을 수 있었다. 또한 P-편광 펌핑 레이저에 대한 내부공진기 진동수 배가된 제2고조파 Nd:YVO$_4$/KTP 녹색 레이저(532 nm)출력 기울기 효율은 23%로 측정되었으며 1000 mW 펌핑 출력에 대하여 빔질 파라메터 M$^2$=1.42인 최대 205 mW의 출력을 얻을 수 있었다.

Effect of oxygen pressure on properties of $NdBa_2Cu_3O_{7-{\delta}}$ films on $SrTiO_3$ (100) substrates grown by pulsed laser deposition

  • Wee, Sung-Hun;Moon, Seung-Hyun;Park, Chan;Yoo, Sang-Im
    • 한국초전도ㆍ저온공학회논문지
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    • 제6권4호
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    • pp.9-12
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    • 2004
  • We report a successful fabrication of high-$J_C$ $NdBa_2Cu_3O_{7-{\delta}}$ (NdBCO) films on (100) $SrTiO_3$ substrates by pulsed laser deposition (PLD) in high oxygen pressures ranging from 400 to 800 mTorr. Fabricated NdBCO films exhibited only c-axis orientation, good out-of-plane and in-plane textures, and also excellent superconducting properties, including critical temperature ($T_C$) and critical current density ($J_C$) of above 90 K and the highest of $3.1MA/cm^2$ at 77 K in self-field, implying that NdBCO is a perspective alternative to YBCO for coated conductor. In low oxygen pressures ranging from 100 to 200 mTorr, however, the films showed a-, c-mixed orientation and degraded $T_{C,zero}$ values due to the formation of $Nd_{1+x}Ba_{2-x}Cu_3O_{7-{\delta}}$-type solid solutions with an excessive substitution of $Nd^{3+}$ ions for the $Ba^{2+}$ sites.

소결방법에 따른 ZrB $_{2 }$ - ZrC 복합체에서의 결정립 방위 분포의 변화 (Grain orientation distribution of the ZrB $_{2 }$ - ZrCcomposite sintered by the different sintering technique)

  • 심승환;;;;오근호;심광보
    • 한국결정성장학회지
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    • 제10권2호
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    • pp.152-158
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    • 2000
  • 상압 소결법(PLS, pressureless sintering) 및 방전가열 소결법(SPS, spark plasma sintering)으로 소결한 {{{{ {ZrB }_{2 } - ZrC }}}} 복합체의 미세구조를 SEM-EBSP 법에 의해 결정기하학적으로 분석하였다. PLS법에 의해 소결된 복합체에서 {{{{ { ZrB}_{2 } }}}}의 (1010) 면은ND(시편에 수직인 방향)로 배향되었고, ZrC 경우 (101) 및 (111)면이 ND방향으로 배향되었다. 한편 SPS법에 위해 소결된 {{{{ { ZrB}_{2 } }}}}의 (0001)A면은 ND방향으로 강하게 배향되었다. ZrC인 경우 (001) 면만이 ND방향으로 배향되었다. PLS법에 의한 소결체의 결정립은 특정방위에 대해 약한 배향을 갖으면서, {{{{ { ZrB}_{2 } }}}}와 ZrC상 계면의 구조적 조화가 우수한 반면, SPS법에 의한 소결체의 결정립들은 특정방향으로 강하게 배향되는 경향을 보인다.

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$(Nd_{1-x}R_x)_2Fe_{14}B$ (R=Y, Pr)의 자기특성 (Magnetic properties of $(Nd_{1-x}R_x)_2Fe_{14}B$ (R=Y, Pr))

  • 김만중;김윤배;김희태;김택기
    • 한국자기학회지
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    • 제8권5호
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    • pp.271-274
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    • 1998
  • 자장중 정렬된(Nd1-xRx)2Fe14B (R=Y, Pr) 다결정 분말을 사용하여 스핀재배열현상과 결정자기이방성을 연구하였다. 이 화합물에서 스핀재배열온도(TSR)는 R=Pr인 경우 0$\leq$x$\leq$0.75 의 조성범위에서 Pr 치환량이 증가함에 따라 $\Delta$TSR=-1.35 K/Pr at.%의 비율로 단순 감소하였으나 R=Y인 경우에는 초기 소량의 감소 후 다시 약간 증가한다. 4.2 K에서 스핀재배열각(SRA)은 Y과 Pr 치환량의 증가에 따라 0$\leq$x$\leq$0.5의 범위에서 $\Delta$SRA=-0.073$^{\circ}$/T at.%와 $\Delta$SRA=-0.258$^{\circ}$/Pr at.% 비율로 감소한다. 4.2 K에서 결정자기이방성상수의 조사결과 R=Y인 경우 x=0.9 이상에서 R=Pr인 경우에는 x=0.8 이상에서 스핀재배열현상이 사라질 것으로 예측되었다.

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피스톤의 제2랜드 길이가 열응력에 미치는 영향 (An Effect of the 2nd Land Length of a Piston on Thermal Stress)

  • 권영웅;박성천
    • 동력기계공학회지
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    • 제12권2호
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    • pp.5-11
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    • 2008
  • An analytical study was performed to have temperature and thermal stress distribution on a piston with the change of the 2nd land length of a piston and the existence of knocking in a cylinder. The result showed that the temperature on the skirt region was about $4\sim10^{\circ}C$ higher than that on the pin region. However the thermal stress on the skirt region was about 4MPa lower than on the pin region. It may be due to the higher heat release rate on the pin boss than on the skirt. The result regarding the variation of the 2nd land length of the piston showed that the temperature distribution on the piston was getting lower and the thermal stress distribution was getting higher as the 2nd land length of the piston was shorter.

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하악 제2대구치의 발치후 제3대구치의 변화에 관한 연구 (THIRD MOLAR CHANGES FOLLOWING LOWER SECOND MOLAR EXTRACTIONS)

  • 홍순창;유영규
    • 대한치과교정학회지
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    • 제17권2호
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    • pp.321-333
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    • 1987
  • The purpose of this study was to observe the changes of the lower 3rd molars following the extraction of the lower 2nd molars by Lateral Cephalograms and Orthopantomograms. The subjects consisted of twenty malocclusion, 7 males 13 females, were 19 year 5 month old at the removal of the lower 2nd molars, 19 year 1 month old at the end of the orthodontic supervision after the removal of the lower 2nd molars (mean age) The obtained results were as follows, 1 It is recommended to extract the lower 2nd molars when the lower 3rd molars are Nolla's Stage 4 or 5 2 With the pre-extraction variables obtained by factor analysis, it was possible to predict the long axis of the lower 3rd molars after 2nd molar extraction. 3 There were no impacted 3rd molars.

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비정상 포텐셜 유동의 패널법 해석에서 포텐셜의 2차 미분값의 수치계산 (Numerical Evaluation of 2nd Derivatives of the Potential in the Panel method for the Unsteady Potential Flow Problem)

  • 양진호;전호환
    • 한국해양공학회지
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    • 제14권3호
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    • pp.41-45
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    • 2000
  • In solving the unsteady potential flow problem of the ship in waves with the panel method, in general one can consider the basic flow as the free stream or double body solution. For the double body solution, the body boundary condition has the 2nd derivatives of the velocity potential. Low order panel methods are known to suffer from the significant error in the 2nd derivatives computed at the body surface. This paper analyzes the numerical error in the 2nd derivatives for a 2-D cylinder and a 3-D sphere problem, and an extrapolation method to obtain the correct derivatives on the body surface is suggested.

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반도체레이저 단면여기 Nd:S-VAP 레이저의 내부공진기 제2고조파 출력 특성 (Output characteristics of intracavity frequency doubling of laser-diode end-pumped Nd:S-VAP laser)

  • 박준학
    • 한국광학회지
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    • 제11권4호
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    • pp.294-298
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    • 2000
  • 반도체레이저로 단면 여기시킨 Nd:VAP 레이저의 내부공진기 제2고조파 출력특성을 조사하였다. 유도방출 단면적과 형광수명의 곱이 커 낮은 발진문턱 특성을 갖는 Nd:S-VAP 매질은 컴팩트한 마이크로칩 레이저에 적합하다. 내부공진기를 이용한 제2고조파 발진문턱에너지가 81 uJ로 측정되어 쉽게 발진됨을 확인하였다. 여기에너지 $2\mu\textrm{J}$에서 제2고조파 에너지 $126\mu\textrm{J}$을 얻었고, 내부공진기 제2고조파의 출력을 계산하여 이론적인 해석 근거를 제시하였다. Q-스위치된 제2고조파 출력은 펄스폭 26ns에 펄스당 에너지 $15\mu\textrm{J}$로 저출력에서도 시.공간적으로 깨끗한 펄스를 얻었으며, $M^2$도 1.47로 우수한 빔 특성을 나타내었다.

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Pressure-Temperature Diagram of Critical Condition for Disproportionation of Nd-Fe-B Alloy in Hydrogen

  • Kwon, H.W.;Kim, D.H.;Yu, J.H.
    • Journal of Magnetics
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    • 제15권4호
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    • pp.155-158
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    • 2010
  • The HDDR (hydrogenation, disproportionation, desorption, and recombination) process can be used as an effective way of converting a no coercivity Nd-Fe-B ingot material, with a coarse $Nd_2Fe_{14}B$ grain structure, to a highly coercive one with a fine grain structure. Careful control of the HDDR process can lead to an anisotropic powder with good $Nd_2Fe_{14}B$ grain texture; the most critical step for inducing texture is disproportionation. The critical conditions (hydrogen pressure and temperature) for the disproportionation reaction of fully hydrogenated $Nd_{12.5}Fe_{81.1-(x+y)}B_{6.4}Ga_xNb_y$ (x = 0 or 0.3, y = 0 or 0.2) alloys, in different atmospheres of pure hydrogen and a mixed gas of hydrogen and argon, was investigated with TPA (thermopiezic analyser). From this, the hydrogen pressure-temperature diagram showing the critical conditions was established. The critical disproportionation temperature of the fully hydrogenated $Nd_{12.5}Fe_{81.1-(x+y)}B_{6.4}Ga_xNb_y$ alloys was slightly increased as the hydrogen pressure decreased in both pure hydrogen and mixed gas. The critical disproportionation temperature of the hydrogenated alloys was higher in the mixed gas than in pure hydrogen. Addition of Ga and Nb increased the critical disproportionation temperature of the fully hydrogenated Nd-Fe-B alloys.

2차원 및 3차원 해석에 의한 토류벽의 변위에 관한 비교 연구 (A Relative Study on the Displacement of Earth Retaining Wall by 2 and 3 Dimentional Analysis)

  • 박춘식;박해찬;김종환;박영준
    • 한국지반공학회:학술대회논문집
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    • 한국지반공학회 2010년도 춘계 학술발표회
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    • pp.801-810
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    • 2010
  • Until now, design of Earth Retaining is practiced by 2nd dimensional analysis for convenience of analysis and time saving. However, the construction field is 3rd dimension, in this study, practised the 3rd dimensional analysis which can reflect the field condition more exactly the scope of earth retaining wall, and researched about the effective and economical way of design, compared and reviewed with the results, by practising both the 2nd and 3rd dimensional analysis. existing 2nd dimension. the depth of excavation, depth of embedded and soil condition. As result, under the whole conditions, more displacement came to appear to the value as result of 3rd dimensional analysis more than the result of 2nd dimensional analysis. Accordingly, the displacement by the 2nd dimension analysis is underestimated. Moreover, results of 2nd and 3rd dimensional analysis, there is no difference at displacement, when the depth of embedded is 0.5H, 1.0H and 1.5H, but Displacement of 1.5H is smaller than 0.5H, 1.0H. That is, the bigger the depth of embedded becomes, the displacement of Earth Retaining Wall appeared smaller. The displacement of earth retaining wall according to depth of excavation appeared bigger, when the depth of excavation is increased. In the meantime, when the soil condition is different, in the 2nd dimensional analysis, the displacement appeared biggest, in case of the clay layer, but in the 3rd dimensional analysis, in the beginning of excavating, the displacement of earth retaining wall appeared bigger in case of clay layer, but as excavating is in progress, the displacement of both compound soil layer and sand layer appeared big.

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