14 research outputs found

    The usefulness of the trouser circumference as a surrogate marker for the waist circumference

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    역학건강증진학과/석사[ν•œκΈ€]λ³Έ μ—°κ΅¬λŠ” λ³΅λΆ€λ―Έλ§Œμ˜ 진단 기쀀인 ν—ˆλ¦¬λ‘˜λ ˆλ₯Ό λŒ€μ‹ ν•  수 μžˆλŠ” ν‘œμ§€μžλ‘œμ„œ λ°”μ§€λ‘˜λ ˆμ˜ μœ μš©μ„±μ„ κ²€μ¦ν•˜κ³ μž ν•˜λŠ” 연ꡬ이닀. 연ꡬ λŒ€μƒμ€ 2009λ…„ 4μ›”λΆ€ν„° 7μ›”κΉŒμ§€ 경기도 μ†Œμž¬ μ’…ν•©λ³‘μ›μ˜ 건강증진센터λ₯Ό λ‚΄μ›ν•œ ν”Όν—˜μžλ₯Ό λŒ€μƒμœΌλ‘œ λΆ„μ„ν•˜μ˜€μœΌλ©° κ·Έ κ²°κ³ΌλŠ” λ‹€μŒκ³Ό κ°™λ‹€. 1. μΈ‘μ •μžλ‚΄ 및 μΈ‘μ •μžκ°„ 였차λ₯Ό ν™•μΈν•˜κΈ° μœ„ν•΄ 21λͺ…μ˜ κ±΄κ°•ν•œ ν”Όν—˜μžλ₯Ό λŒ€μƒμœΌλ‘œ 5λͺ…μ˜ μΈ‘μ •μžκ°€ ν—ˆλ¦¬λ‘˜λ ˆλ₯Ό μΈ‘μ •ν•˜λŠ” μ‹œν—˜μ—μ„œ ν—ˆλ¦¬λ‘˜λ ˆμ— λŒ€ν•œ μΈ‘μ •μžκ°„ κΈ‰λ‚΄μƒκ΄€κ³„μˆ˜λŠ” 0.993(0.989-0.996, 95% 신뒰ꡬ간)으둜 μΈ‘μ •μžκ°„ μ˜€μ°¨λŠ” ν†΅κ³„μ μœΌλ‘œ μœ μ˜ν•˜μ§€ μ•Šμ•˜λ‹€. μΈ‘μ •μžλ‚΄ 였차 μ—­μ‹œ 5λͺ…μ˜ μΈ‘μ •μžμ—μ„œ λͺ¨λ‘ ν†΅κ³„μ μœΌλ‘œ μœ μ˜ν•˜μ§€ μ•Šμ•˜λ‹€. 2. 연ꡬ에 λ™μ˜ν•œ ν”Όν—˜μžλŠ” 총 733λͺ…μœΌλ‘œ λ‚¨μžκ°€ 422λͺ…(57.49%), μ—¬μžκ°€ 311λͺ…(42.51%)μ΄μ—ˆκ³  연령은 18μ„Έμ—μ„œ 79세에 걸쳐 λΆ„ν¬ν•˜μ˜€μœΌλ©° 평균 연령은 45.43 Β± 10.19μ„Έμ˜€λ‹€. 이 쀑 볡뢀 λΉ„λ§Œμ— ν•΄λ‹Ήν•˜λŠ” ν”Όν—˜μžλŠ” λ‚¨μž 124(29.38%)λͺ…, μ—¬μž 84(10.93%)λͺ…μ΄μ—ˆμœΌλ©° λŒ€μ‚¬ 증후ꡰ에 ν•΄λ‹Ήν•˜λŠ” ν”Όν—˜μžλŠ” λ‚¨μž 83(19.67%)λͺ…, μ—¬μž 24λͺ…(7.72%)μ΄μ—ˆλ‹€. 3. λ‚¨μžμ˜ ν—ˆλ¦¬λ‘˜λ ˆμ˜ 평균은 86.33 Β± 7.40cm, μ—¬μžμ˜ ν—ˆλ¦¬λ‘˜λ ˆλŠ” 79.51 Β± 8.36cmμ΄μ—ˆλ‹€. 섀문을 톡해 ν™•μΈν•œ λ°”μ§€λ‘˜λ ˆμ˜ 평균은 λ‚¨μžμ—μ„œ 85.40 Β± 5.66cm으둜 μ‹€μΈ‘ ν—ˆλ¦¬λ‘˜λ ˆμ™€ μ°¨μ΄λŠ” 0.94 Β± 4.48cmμ΄μ—ˆκ³  μ—¬μžμ—μ„œλŠ” 72.96 Β± 7.06cm으둜 μ‹€μΈ‘ ν—ˆλ¦¬λ‘˜λ ˆμ™€μ˜ μ°¨μ΄λŠ” 6.55 Β± 6.46cmμ΄μ—ˆλ‹€. λ‚¨μžμ™€ μ—¬μžμ—μ„œ ν—ˆλ¦¬λ‘˜λ ˆμ™€ λ°”μ§€λ‘˜λ ˆμ˜ 차이값은 ν†΅κ³„μ μœΌλ‘œ μœ μ˜ν•œ 차이가 μžˆμ—ˆλ‹€(P<.001) 4. ν—ˆλ¦¬λ‘˜λ ˆμ™€ λ°”μ§€λ‘˜λ ˆμ˜ μƒκ΄€κ΄€κ³„λŠ” 남녀 μ „μ²΄μ—μ„œλŠ” μƒκ΄€κ³„μˆ˜κ°€ 0.75(P< .001)μ΄μ—ˆκ³ , λ‚¨μžμ—μ„œ 0.80(P<.001)으둜 μ—¬μžμ˜ 0.66(P<.001)보닀 λ†’μ•˜λ‹€. 5. μ‹€μΈ‘ ν—ˆλ¦¬λ‘˜λ ˆλ₯Ό κΈ°μ€€μœΌλ‘œ λ³΅λΆ€λΉ„λ§ŒμΈ μ‚¬λžŒλ“€μ€ 그렇지 μ•Šμ€ μ‚¬λžŒμ— λΉ„ν•΄ 남녀 λͺ¨λ‘μ—μ„œ λŒ€μ‚¬μ¦ν›„κ΅°μ˜ ꡬ성 μš”μ†ŒμΈ 쀑성지방, κ³ λ°€λ„μ½œλ ˆμŠ€ν…Œλ‘€, μˆ˜μΆ•κΈ° ν˜ˆμ••, 이완기 ν˜ˆμ••μ˜ 평균을 λΉ„κ΅ν–ˆμ„ λ•Œ ν†΅κ³„μ μœΌλ‘œ μœ μ˜ν•˜κ²Œ 차이가 μžˆμ—ˆκ³ (P<0.05) κ³΅λ³΅ν˜ˆλ‹Ήμ€ μ—¬μžμ—μ„œλ§Œ μœ μ˜ν•œ 차이가 μžˆμ—ˆλ‹€(P=0.001). λ°”μ§€λ‘˜λ ˆλ₯Ό κΈ°μ€€μœΌλ‘œ ν•œ λΉ„κ΅μ—μ„œλ„ 남녀 λͺ¨λ‘ 쀑성지방, κ³ λ°€λ„μ½œλ ˆμŠ€ν…Œλ‘€, μˆ˜μΆ•κΈ° ν˜ˆμ••, 이완기 ν˜ˆμ••μ—μ„œ ν†΅κ³„μ μœΌλ‘œ μœ μ˜ν•œ 차이가 μžˆμ—ˆκ³ (P<0.05), μ—­μ‹œ κ³΅λ³΅ν˜ˆλ‹Ήμ€ μ—¬μžμ—μ„œλ§Œ μœ μ˜ν•œ 차이가 μžˆμ—ˆλ‹€(P=0.046). 6. ν—ˆλ¦¬λ‘˜λ ˆμ™€ λ°”μ§€λ‘˜λ ˆμ˜ 차이값은 남,λ…€ λͺ¨λ‘μ—μ„œ ν—ˆλ¦¬λ‘˜λ ˆμ— 따라 ν†΅κ³„μ μœΌλ‘œ μœ μ˜ν•œ 차이가 μžˆμ—ˆλ‹€(P<.001). λ˜ν•œ νˆ¬ν‚€μ˜ 닀쀑 비ꡐ κ²°κ³Ό ν—ˆλ¦¬λ‘˜λ ˆ 별 각 κ·Έλ£Ήλ§ˆλ‹€ ν—ˆλ¦¬λ‘˜λ ˆμ™€ λ°”μ§€λ‘˜λ ˆμ˜ 차이값에 차이가 μžˆμ—ˆλ‹€. λ‚˜μ΄μ— 따라 μ—¬μžμ—μ„œλŠ” κ·Έλ£Ήλ³„λ‘œ ν—ˆλ¦¬λ‘˜λ ˆμ™€ λ°”μ§€λ‘˜λ ˆμ˜ 차이값에 λŒ€ν•œ 차이가 μ—†μ—ˆμœΌλ‚˜(P=0.204) λ‚¨μžμ—μ„œλŠ” 40λŒ€ 미만 κ·Έλ£Ήκ³Ό κ·Έ μ΄μƒμ˜ κ·Έλ£Ήμ—μ„œ μœ μ˜ν•œ 차이가 μžˆμ—ˆλ‹€(P=0.015). λ³Έ 연ꡬ결과λ₯Ό μ’…ν•©ν•˜λ©΄ ν—ˆλ¦¬λ‘˜λ ˆμ™€ λ°”μ§€λ‘˜λ ˆμ˜ μƒκ΄€κ΄€κ³„λŠ” μ—¬μžλ³΄λ‹€ λ‚¨μžμ—μ„œ λ†’κ³  ν—ˆλ¦¬λ‘˜λ ˆμ™€ λ°”μ§€λ‘˜λ ˆμ˜ 차이값도 λ‚¨μžκ°€ μ—¬μžλ³΄λ‹€ 적어 μ—¬μžμ—μ„œλ³΄λ‹€ λ‚¨μžμ—μ„œ λ°”μ§€λ‘˜λ ˆκ°€ ν—ˆλ¦¬λ‘˜λ ˆλ₯Ό 잘 λŒ€ν‘œν•œλ‹€κ³  ν•  수 μžˆλ‹€. 특히 ν—ˆλ¦¬λ‘˜λ ˆ 90cm미만, 40μ„Έ 이상 λ‚¨μžμ—μ„œλŠ” λ°”μ§€λ‘˜λ ˆκ°€ ν—ˆλ¦¬λ‘˜λ ˆμ˜ μ€‘μš”ν•œ λŒ€λ¦¬ ν‘œμ§€μžκ°€ 될 수 μžˆλ‹€. ν•˜μ§€λ§Œ ν—ˆλ¦¬λ‘˜λ ˆκ°€ 컀질수둝, μ—¬μžμΌμˆ˜λ‘ ν—ˆλ¦¬λ‘˜λ ˆμ™€ λ°”μ§€λ‘˜λ ˆμ˜ 차이가 컀져 이에 λŒ€ν•œ 원인과 차이값에 영ν–₯을 쀄 수 μžˆλŠ” μΆ”κ°€ λ³€μˆ˜μ— λŒ€ν•œ 연ꡬ가 ν•„μš”ν•˜λ‹€. [영문]ope

    The Microhardness and the degree of conversion of light cured composite resin and dual cured resin cements under porcelain inlay

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    ν•™μœ„λ…Όλ¬Έ(박사)--μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› :μΉ˜μ˜ν•™κ³Ό μΉ˜κ³Όλ³΄μ‘΄ν•™μ „κ³΅,1999.Docto

    Pattern Filling Using Pulse and Pulse-Reverse Current in Damascene Cu Metallization

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    ν•™μœ„λ…Όλ¬Έ(석사) --μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› :화학생물곡학뢀,2007.Maste

    κ³ μ •μ„± 보철물을 μ§€μ§€ν•˜λŠ” 지λ₯΄μ½”λ‹ˆμ•„ μž„ν”Œλž€νŠΈ μ§€λŒ€μ£Όμ˜ μƒμ‘΄μœ¨κ³Ό 합병증에 κ΄€ν•œ 연ꡬ : 5년이상 follow-up 쑰사

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    ν•™μœ„λ…Όλ¬Έ (석사)-- μ„œμšΈλŒ€ν•™κ΅ λŒ€ν•™μ› : μΉ˜μ˜ν•™κ³Ό, 2011.2. ν•œμ€‘μ„.Maste

    Multidimensional Interpolation Method for Simulating Photodynamics in Complex Environment

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    DoctorSimulating photodynamics on the biological system is one of the most challenging tasks in the field of computational chemistry. The challenge includes attaining a reliable and efficient treatment of multiple electronic states. Toward the purpose, quantum mechanics / molecular mechanics (QM/MM) calculations are often conducted in a β€œdirect dynamics” manner. To avoid such direct quantum chemical calculations, one must somehow model the associated multiple potential energy surfaces (PESs). The interpolation of PES is an attractive path toward that end, as it can describe the energy landscape with minimum biases in parameter estimations. It can also be coupled as a multiscale approach in combination with MM approaches. The resultant scheme, called interpolation mechanics / molecular mechanics (IM/MM), can be a useful tool for studying the dynamics of complex systems. In this thesis, a short review about the formal framework of IM/MM method will be presented in Theoretical Background (Chapter 2). After that, two studies related to IM/MM method will be presented: atomic partial charge interpolation as a tool for modeling charge flux (Chapter 3) and IM/MM PES construction of photoactive yellow protein (Chapter 4). The former mainly deals with the methodological development toward more realistic IM/MM PES. The latter describes the application of IM/MM to the excited state dynamics of the photoactive yellow protein. Also, the limitations and potential resolutions will be discussed in Conclusions and Perspectives (Chapter 5).생물학적 μ‹œμŠ€ν…œμ—μ„œ μΌμ–΄λ‚˜λŠ” 광동역학을 λͺ¨μ‚¬ν•˜λŠ” 것은 μ „μ‚° ν™”ν•™ λΆ„μ•Όμ—μ„œ κ°€μž₯ μ–΄λ €μš΄ 과제 쀑 ν•˜λ‚˜μ΄λ‹€. 이 κ³Όμ œμ—λŠ” μ—¬λŸ¬ μ „μž μƒνƒœμ— λŒ€ν•œ μ •ν™•ν•˜κ³  효율적인 계산법이 μš”κ΅¬λ˜κΈ° λ•Œλ¬Έμ΄λ‹€. 이λ₯Ό μœ„ν•΄, μ–‘μž μ—­ν•™/λΆ„μž μ—­ν•™ 계산이 직접 μ—­ν•™ 방식 (μ „μ‚° λͺ¨μ‚¬μ˜ 맀 μ‹œκ°„ κ±ΈμŒλ§ˆλ‹€ 계산을 λ°˜λ³΅ν•˜λŠ” κ²ƒμœΌλ‘œ 계산 뢀담이 맀우 큰 방식)으둜 μˆ˜ν–‰λ˜μ–΄ μ™”λ‹€. μ΄λŸ¬ν•œ 직접 μ—­ν•™ 계산을 ν”Όν•˜κΈ° μœ„ν•΄μ„œλŠ” μ–΄λ–»κ²Œλ“  μ—¬λŸ¬ μ „μž μƒνƒœλ₯Ό κ°–λŠ” 닀쀑 νΌν…μ…œ μ—λ„ˆμ§€ ν‘œλ©΄ (PES; potential energy surface)을 λͺ¨λΈλ§ν•΄μ•Ό ν•œλ‹€. 이 λ•Œ, PES 내삽법은 맀개 λ³€μˆ˜λ₯Ό μ΄μš©ν•œ λͺ¨λΈλ§μ—μ„œ λ°œμƒν•  수 μžˆλŠ” λ°”μ΄μ–΄μŠ€λ₯Ό μ΅œμ†Œν™”ν•˜λ©΄μ„œ PESλ₯Ό κΈ°μˆ ν•  수 μžˆλ‹€λŠ” μž₯점을 가지고 μžˆλ‹€. λ˜ν•œ PES 내삽법이 기쑴의 λΆ„μž μ—­ν•™ 방식과 ν•¨κ»˜ 닀쀑 μŠ€μΌ€μΌ λ°©μ‹μœΌλ‘œ κ²°ν•©λ˜λ©΄, λ‚΄μ‚½ μ—­ν•™/λΆ„μž μ—­ν•™ (IM/MM; interpolation mechanics/molecular mechanics) 방법이 μ–»μ–΄μ§€λŠ”λ°, 이 방법은 λ³΅μž‘ν•œ μ‹œμŠ€ν…œμ˜ 동역학을 이둠적으둜 μ—°κ΅¬ν•˜λŠ” 데에 μœ μš©ν•œ 도ꡬ가 될 수 μžˆλ‹€. 이 λ…Όλ¬Έμ˜ 이둠적 λ°°κ²½ (제 2μž₯)μ—μ„œλŠ” λ¨Όμ € IM/MM을 κ΅¬μ„±ν•˜λŠ” μˆ˜ν•™μ  틀이 짧게 검토될 것이닀. κ·Έ ν›„, IM/MM 방법에 κΈ°λ°˜ν•œ 두 가지 연ꡬ가 μ œμ‹œλ  것이닀. 제 3μž₯μ—μ„œλŠ” μ „ν•˜ ν”ŒλŸ­μŠ€ λͺ¨λΈλ§μ„ μœ„ν•œ λ„κ΅¬λ‘œμ„œμ˜ μ›μž λΆ€λΆ„ μ „ν•˜ 내삽법이, 제 4μž₯μ—μ„œλŠ” κ΄‘ν™œμ„± 황색 λ‹¨λ°±μ§ˆμ˜ IM/MM PES ꡬ좕이 μ œμ‹œλ  것이닀. μ „μžλŠ” IM/MM λ°©λ²•λ‘ μ˜ 정확도λ₯Ό 올리기 μœ„ν•œ 이둠적 κ°œλ°œμ„ λ‹€λ£¨λŠ” 것이며, ν›„μžλŠ” κ΄‘ν™œμ„± 황색 λ‹¨λ°±μ§ˆμ˜ λ“€λœ¬ μƒνƒœ 동역학에 λŒ€ν•΄ IM/MM 방법둠을 μ‘μš©ν•œ κ²°κ³Όλ₯Ό κΈ°μˆ ν•˜λŠ” 것이닀. 두 μ—°κ΅¬μ˜ ν•œκ³„ 및 이에 λŒ€ν•œ 잠재적인 연ꡬ μ£Όμ œλ“€μ€ κ²°λ‘  및 전망 (제 5 μž₯)μ—μ„œ λ…Όμ˜ 될 것이닀
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