31 research outputs found
Measurement of maxillary sinus volume using computed tomography
์น์ํ๊ณผ/์์ฌ[ํ๊ธ]
์ ์์ ์ธ ์์
๋ ํฌ๊ธฐ์ ๊ดํ ํ์ค์น๋ ์์
๋์ ๋น์ ์์ ์ํ๋ฅผ ํ๊ฐํ๋๋ฐ ๋์์ ์ฃผ๊ณ , ์์
๋์ด ํฌํจ๋ ์ธ๊ณผ์ ์์ ์ธ ๊ฒฝ์ฐ ์์
๊ณจ์ ์ ํํ๊ฒ ์๋ณตํ๊ณ ์ ํ ๊ฒฐ๊ณผ๋ฅผ ํ๊ฐํ๋๋ฐ์๋ ์ค์ํ๋ค.
์ด์ ์ ์๋ 20์ธ ์ด์ ํ๊ตญ์ธ ์ ์ ์ฑ์ธ ์์
๋์ ํก๋จ ํญ๊ฒฝ, ์ ํ ํญ๊ฒฝ ๋ฐ ๊ณ ๊ฒฝ์ ์ธก์ ํ์ฌ ์ฒด์ ์ ๊ตฌํ ๋ค ์์
๋ ๊ฐ๊ฐ์ ๊ณ์ธก์น๊ฐ ์์
๋ ์ฒด์ ๊ณผ ๊ฐ๋ ์๊ด ๊ด๊ณ๋ฅผ ํ๊ฐํ๊ณ ์ฑ๋ณ, ์ข์ฐ๋ณ ์์
๋ ํฌ๊ธฐ์ ์ฐจ์ด๋ฅผ ์์๋ด์ผ๋ก์จ ํ๊ตญ์ธ ์ ์ ์ฑ์ธ ์์
๋ ํฌ๊ธฐ์ ํ์ค์น๋ฅผ ์ ์ํ๊ณ ์ ํ์๋ค. 1997๋
2์๋ถํฐ 1999๋
7์๊น์ง ์ฐ์ธ๋ํ๊ต ์น๊ณผ๋ํ๋ณ์ ์น๊ณผ๋ฐฉ์ฌ์ ๊ณผ์์ ์ ์ฐํ๋จ์ธต์ฌ์ง์ ์ดฌ์ํ 20์ธ ์ด์ ์ฑ์ธ ํ์ ์ค ์์
๋๋ด์ ํน๋ณํ ์ฆ์์ด๋ ์ค๊ฒฉ(septa)์ด ์๊ณ , ๊ณจ์ ์ด๋ ์ผ์ฆ, ์ข
์ ๋ฑ์ ๋ณ๋ณ๋ ์์ผ๋ฉฐ, ์์์ ์ผ๋ก ์ฌํ ๋น๋์นญ ์๊ฒฌ์ด๋ ์
์๋ฉด๋ถ์ ์์ ์ ๋ฐ์ ๋ณ๋ ฅ์ด ์๋ 52๋ช
ํ์(์ด ์์
๋ ์ 95๊ฐ๋)์ ์ ์ฐํ๋จ์ธต์ฌ์ง์ ๋์์ผ๋ก ํํฅ์ ์ผ๋ก ๊ณ ์ฐฐ, ๋ถ์ํ์ฌ ๋ค์๊ณผ ๊ฐ์ ๊ฒฐ๊ณผ๋ฅผ ์ป์๋ค.
1. ์ ์ฒด ์์
๋ ํก๋จ ํญ๊ฒฝ, ์ ํ ํญ๊ฒฝ, ๊ณ ๊ฒฝ, ์ฒด์ ์ ํ๊ท ๊ฐ์ ๊ฐ๊ฐ 28.33 mm,39.69 mm, 46.60 mm, 21.90 cm** 3์ด์๋ค. ๋ค ๊ณ์ธก ํญ๋ชฉ ๋ชจ๋ ์ ๋ฐ์ ์ผ๋ก ๋จ์๊ฐ ์ฌ์์ ๋นํด ๋ค์ ํฐ ๊ฒฝํฅ์ด ์์์ผ๋ฉฐ, ํญ๊ฒฝ ๋ฐ ๊ณ ๊ฒฝ์์๋ ์ฑ๋ณ๊ฐ์ ํต๊ณํ์ ์ผ๋ก ์ ์์ฑ์๋ ์ฐจ์ด๊ฐ ์์์ผ๋, ์ฒด์ ์์๋ ํต๊ณํ์ ์ผ๋ก ์ ์์ฑ์๋ ์ฐจ์ด๊ฐ ์์๋ค(p<0.05).
2. ์ข์ฐ๋ณ ์ฐจ์ด๋ฅผ ๋ณด๋ฉด ์์
๋ ์ ํ ํญ๊ฒฝ, ๊ณ ๊ฒฝ, ์ฒด์ ์์ ํต๊ณํ์ ์ผ๋ก ์ ์์ฑ์๋ ์ฐจ์ด๊ฐ ์์์ผ๋ฉฐ, ํก๋จ ํญ๊ฒฝ์์ ํต๊ณํ์ ์ผ๋ก ์ ์์ฑ์๋ ์ฐจ์ด๊ฐ ์์์ผ๋(p<0.05), ๊ทธ ์ฐจ์ด์ ํ๊ท ๊ฐ์ 0,84 mm์๋ค. ๋ค ๊ณ์ธก ํญ๋ชฉ ๋ชจ๋ ์ข์ฐ๊ฐ์ ํต๊ณํ์ ์ผ๋ก ์ ์์ฑ์๋ ์๊ด ๊ด๊ณ๊ฐ ์์๋ค(p<0.0001).
3. ์์
๋์ ํก๋จ ํญ๊ฒฝ, ์ ํ ํญ๊ฒฝ, ๊ณ ๊ฒฝ์ ๋ชจ๋ ์์
๋์ ์ฒด์ ๊ณผ ํต๊ณํ์ ์ผ๋ก ์ ์์ฑ์๋ ์๊ด ๊ด๊ณ๋ฅผ ๋ณด์๋ค(p<0.0001).
๊ฒฐ๋ก ์ ์ผ๋ก ํ๊ตญ์ธ ์ ์ ์ฑ์ธ์ ์์
๋์ ์ฑ๋ณ๊ฐ์๋ ์ ๋ฐ์ ์ผ๋ก ๋จ์๊ฐ ์ฌ์์ ๋นํด ๋ค์ ํฐ ๊ฒฝํฅ์ด ์์๊ณ , ์ข์ฐ๊ฐ์๋ ํก๋จ ํญ๊ฒฝ์ ์ ์ธํ๊ณ ๋ชจ๋ ๊ณ์ธก์น์์ ํต๊ณํ์ ์ผ๋ก ์ ์์ฑ์๋ ์ฐจ์ด๊ฐ ์์์ผ๋ฉฐ, ๋ค ๊ณ์ธก์น ๋ชจ๋ ์ข์ฐ๊ฐ์ ์ ์์ฑ์๋ ์๊ด ๊ด๊ณ๊ฐ ์์๋ค.
๋ฐ๋ผ์ ํธ์ธก์ผ๋ก ์์
๋์ ๊ณผ์ฑ์ฅ์ด๋ ์ด์ฑ์ฅ์ด ๊ด์ฐฐ๋๋ค๋ฉด ์์
๋ ํฌ๊ธฐ์ ์ํฅ์ ๋ฏธ์น ์ ์๋ ์ด๋ค ์์
๋ ๋ณ๋ณ์ด๋ ๋ฐ์ก์ฑ ์ด์์ ์๊ฐํด ๋ณผ ์ ์์ ๊ฒ์ผ๋ก ์ฌ๋ฃ๋๋ค. ๋ํ ์์
๋ ์ฒด์ ๊ณผ ๋๋จธ์ง ์ธ ๊ณ์ธก์น๊ฐ์ ๊ฐ๊ฐ ์ ์์ฑ์๋ ์๊ด ๊ด๊ณ๊ฐ ์์์ผ๋ฏ๋ก ์์
๋ ํญ๊ฒฝ ๋ฐ ๊ณ ๊ฒฝ์ด ํฌ๋ฉด ์ฒด์ ๋ ํด ๊ฒ์ผ๋ก ์์ํ ์ ์์ ๊ฒ์ด๋ค.
[์๋ฌธ]
A standard value for the size of the normal maxillary sinus is important to evaluate the state of the maxillary sinus, as well as to precisely reduce the maxilla and to evaluate the results of an operation involving the maxillary sinus.
This study was carried out to propose a standard value for the maxillary sinus volume of a normal Korean adult by measuring the width and height of the sinus and analyzing their correlation with the sinus volume and the difference of the maxillary sinus size respectively between sex, and on the right and left sides.
Fifty-two patients(a total of 95 maxillary sinuses) out of adult patients aged 20 years or over who had taken CT in the Department of Dental Radiology, Yonsei University, Dental Hospital, between February 1997 and July 1999 who were without
specific symptom, prominent bony septa, fracture, inflammation, tumor, clinical asymmetry and no history of orthognathic surgery were retrospectively analyzed.
The results were as follows :
1. The mean transverse width, antero-posterior width, height and volume of the normal Korean adult's maxillary sinuses were 28.33 mm, 39.69 mm, 46.60mm and 21.90 cm**3, respectively. In all four measurements, the mean values in males were larger than in females. There were no significant sex differences in the mean width and height. However, in the mean volume, a significant difference was observed between the sex(p<0.05).
2. In the mean antero-posterior width, height and volume of the maxillary sinus, no significant difference was observed between the right and left side. In the mean transverse width, however, a significant difference was observed(p<0.05), but the mean difference between the two sides was 0.84mm. All four measurements showed a significant correlation between the right and left sides(p<0.0001),
3. The widths and height of the maxillary sinus all showed a significant correlation with the sinus volume(p<0.0001).
Conclusively, in the Korean normal adult's maxillary sinus, males tended to be larger than females. Except far the transverse width, all of the measurements showed no significant difference between the right and left side, but significant correlations in the four measurements between both sides were observed. Thus, the
overgrowth or undergrowth in the unilateral maxillary sinus may suggest a certain pathosis or developmental abnormalities in the maxillary sinus.
Also there were a number of significant correlations between the width, height and volume of the maxillary sinus. So, we can expect that maxillary sinus volume is also large if the width and height are large.ope
๊ด์๊ทน๋ฐ๊ด์ ๋๊ณ(OSLD)์ธก์ ๋ฒ๊ณผ ๋ชฌํ ์นด๋ฅผ๋ก ์ฐ์ถ๋ฒ(MC)์ ์ํ ์ฝ๋น์ํฐ์ ์ ํจ์ ๋ ํ๊ฐ
์น์ํ์ ๋ฌธ๋ํ์Objective: The aim of this study was to evaluate the effective dose of three different cone beam computed tomography (CBCT) units with optically stimulated luminescence dosimeters (OSLD). Also, this dosimetric measurement method was compared with Monte Carlo (MC) simulation in Alphard 3030 CBCT unit. Through the measurement process and obtained value, more practical and efficient method in acquiring the effective dose of a CBCT would be suggested. Materials and Methods: Twenty-two optically stimulated luminescence dosimeters (OSLD) were calibrated and equipped in human anthropomorphic phantom of head and neck. The phantom with dosimetry was exposed respectively with C, P and I modes of Alphard 3030 (Asahi Roentgen Ind., Co. Ltd, Kyoto, Japan); Large Jaw and Jaw modes of RAYSCAN ฮฑ+ (Ray Co. Ltd, Hwaseong-si, Korea); Facial and Dual Jaw modes of CS9300 (Carestream Dental LLC, Atlanta, Georgia). Dose recorded in dosimetry was obtained and organ dose as well as effective dose were obtained in each examination mode of 3 CBCT units. The organ and effective dose were also obtained with MC simulation on three examination modes of Alphard 3030 CBCT unit. For MC simulation, PCXMC software (STUK, Helsinki, Finland) was used and dose-area-product (DAP) value was measured with DAP meter. Results: The effective dose was the highest in C mode, Alphard 3030 and the lowest in Dual jaw mode, CS9300. When comparing the 10 x10 cm FOV mode of all 3 CBCT units, the effective dose was higher in order of Alphard 3030 (258.8 ยตSv), RAYSCAN ฮฑ+ (213.8 ยตSv), and CS9300 (90.7 ยตSv). The organ dose was the highest in salivary gland and the lowest in bone marrow in the same FOV mode of 3 CBCT units. When compared the result of OSLD in Alphard 3030 with MC simulation, percent difference of the effective dose was 9.8~23.4%. Overall organ dose distribution was consistent in all different examination modes of Alphard 3030 CBCT unit. Conclusion: The effective dose showed tendency of increasing as FOV increased regardless of the CBCT model. In addition, the effective dose varies depending on several other factors such as exposure conditions and geometry of the CBCT, thus the effective dose of various equipment should be examined in the future. Also, MC simulation is expected to be convenient assessment method because it was similar to the OSLD measured value according to the examination modes.
๋ชฉ์ : ๊ด์๊ทน๋ฐ๊ด์ ๋๊ณ(OSLD)๋ฅผ ์ด์ฉํ์ฌ ์ธ ์ข
๋ฅ์ ์ฝ๋น์ํฐ์์ ์ ํจ์ ๋์ ์ธก์ ํ๊ณ , Alphard 3030 ์ฝ๋น์ํฐ์์ OSLD ์ธก์ ๊ฐ๊ณผ ๋ชฌํ
์นด๋ฅผ๋ก(MC) ์๋ฎฌ๋ ์ด์
์ฐ์ถ๊ฐ์ ๋น๊ตํ๋ ๊ฒ์ด๋ค. ์ด๋ฅผ ํตํด ์ฝ๋น์ํฐ ์ ํจ์ ๋์ ํ๋ํ๊ธฐ ์ํ ๋ณด๋ค ์ค์ฉ์ ์ด๊ณ ํจ์จ์ ์ธ ๋ฐฉ๋ฒ์ ์ ์ํ๊ณ ์ ํ๋ค. ์ฌ๋ฃ ๋ฐ ๋ฐฉ๋ฒ: ์ด๊ธฐ ๋ณด์ ์ ๊ฑฐ์น 22๊ฐ์ OSLD๋ฅผ ์ฑ์ธ ๋๊ฒฝ๋ถ๋ฅผ ์ฌํํ ATOM (CIRS, Norfolk, VA) ํฌํ
์ ์ ํด์ง ์์น์ ๊ฐ๊ฐ ์ฝ์
ํ์๋ค. ์ค๋น๋ ํฌํ
์ ์ธ ์ข
๋ฅ์ ์ฝ๋น์ํฐ๋ฅผ ์ด์ฉํ์ฌ ์ ์กฐ์ฌ๊ฐ ์ ์ํ ๋
ธ์ถ์กฐ๊ฑด์ผ๋ก ์ดฌ์ํ์๋ค. Alphard 3030 ์ฝ๋น์ํฐ(Asahi Roentgen Ind., Co. Ltd, Kyoto, Japan)์์ C, P, I 3๊ฐ์ง ๋ชจ๋, RAYSCAN ฮฑ+ ์ฝ๋น์ํฐ(Ray Co. Ltd, Hwaseong-si, Korea)์์ Large jaw, jaw 2๊ฐ์ง ๋ชจ๋, CS9300 ์ฝ๋น์ํฐ(Carestream Dental LLC, Atlanta, Georgia)์์ Facial, Dual jaw 2๊ฐ์ง ๋ชจ๋๋ก ๊ฐ๊ฐ ์ดฌ์ํ์๋ค. ๋ชจ๋ ๋ณ๋ก OSLD ์ธก์ ๊ฐ์ ์ป๊ณ , ์ฅ๊ธฐ ํก์์ ๋๊ณผ ์ ํจ์ ๋์ ์ฐ์ถํ์๋ค. ๋ํ Alphard 3030์ 3๊ฐ์ง ๋ชจ๋์์๋ ์ ๋๋ฉด์ ๊ณฑ์ธก์ ๊ณ DAP meter (VacuDAPTM; VacuTec Meรtechnik GmbH, Dresden, Germany)๋ก ๋
ธ์ถ์ ๋์ ์ธก์ ํ์๋ค. ์ด ๊ฐ์ ํตํด PCXMC ์ํํธ์จ์ด(STUK, Helsinki, Finland)๋ฅผ ์ฌ์ฉํ์ฌ ๋ชฌํ
์นด๋ฅผ๋ก ์ฐ์ถ๋ฒ์ผ๋ก ์ฅ๊ธฐ ํก์์ ๋๊ณผ ์ ํจ์ ๋์ ํ๋ํ์๋ค. OSLD์ MC ๋ ๋ฐฉ๋ฒ ๊ฐ์ ์ ํจ์ ๋ ์ฐจ์ด๋ฅผ % ์ค์ฐจ๋ก ๋น๊ตํ์๋ค. ๊ฒฐ๊ณผ: OSLD๋ก ์ธก์ ํ ์ ํจ์ ๋์ Alphard 3030 C ๋ชจ๋์์ ๊ฐ์ฅ ๋์๊ณ (599.0 ยตSv), CS 9300 Dual jaw ๋ชจ๋์์ ๊ฐ์ฅ ๋ฎ์๋ค (90.7 ยตSv). ์กฐ์ฌ์ผ ํฌ๊ธฐ๊ฐ 10ร10 cm์ผ๋ก ๋์ผํ ๋ชจ๋ ๊ฐ์ ์ ํจ์ ๋์ ๋น๊ตํ๋ฉด Alphard 3030 (258.8 ยตSv), RAYSCAN ฮฑ+ (213.8 ยตSv), CS9300 (90.7 ยตSv) ์์๋๋ก ๋๊ฒ ๋ํ๋ฌ๋ค. ์ฅ๊ธฐ๋ณ ํก์์ ๋์ ์ฝ๋น์ํฐ์ ์ข
๋ฅ์ ์๊ด์์ด ํ์ก์ ์์ ๊ฐ์ฅ ๋์๊ณ , ๊ณจ์์์ ๊ฐ์ฅ ๋ฎ์๋ค. Alphard 3030 ์ฝ๋น์ํฐ์ OSLD ์ธก์ ๊ฐ๊ณผ MC ์ฐ์ถ๊ฐ์ ๋น๊ตํด๋ณด๋ฉด, ์ ํจ์ ๋์ ๋ ๋ฐฉ๋ฒ ๊ฐ ํผ์ผํธ ์ค์ฐจ๋ 9.8~23.4 %๋ฅผ ๋ณด์๋ค. ๋ ๋ฐฉ๋ฒ ๊ฐ์ ์ฅ๊ธฐ๋ณ ํก์์ ๋์ ์ ๋ฐ์ ์ธ ๋ถํฌ๋ Alphard 3030 ์ฝ๋น์ํฐ์ ๊ฒ์ฌ ๋ชจ๋์ ์๊ด์์ด ๋น์ทํ ์์์ ๋ณด์๋ค. ๊ฒฐ๋ก : MC ์ฐ์ถ๊ฐ์ ๊ฒ์ฌ ๋ชจ๋์ ๋ฐ๋ฅธ OSLD ์ธก์ ๊ฐ๊ณผ ์ ์ฌํ ์์ค์ ๊ฒฐ๊ณผ๋ฅผ ๋ณด์๋ค. ๋ฐ๋ผ์ MC ์ฐ์ถ๋ฒ์ ์์์์ ์ฌ์ฉํ ์ ์๋ ํธ๋ฆฌํ ๋ฐฉ์ฌ์ ๋์ธก์ ๋ฐฉ๋ฒ์ผ๋ก ๊ธฐ๋๋๋ค. ์ค์ฌ๋จ์ด: ๋ชฌํ
์นด๋ฅผ๋ก๋ฐฉ๋ฒ, ์ ๋์ธก์ ๋ฒ, ์ฝ๋น์ํฐ, ๊ด์๊ทน๋ฐ๊ด์ ๋๊ณopen๋ฐ
๊ณ ๊ฐ๋๊ฐ ํจ ๋ถ์ฌ์ ๋นํ์ฑ ํก๋นํ๋ฆผ์ข๊ตด ๊ฑฐ๋
ํ์๋
ผ๋ฌธ (๋ฐ์ฌ)-- ์์ธ๋ํ๊ต ๋ํ์ : ๊ฑด์ถํ๊ณผ, 2015. 2. ์ด์ฒ ํธ.This research focuses on the inelastic behavior of structural I-shaped members fabricated from 800MPa high strength steel (HSA800). HSA800, a new generation of high performance steel, produced by thermo-mechanical controlling (TMC) process, has the advantages to acquire the high strength as well high toughness and relatively low carbon equivalent value (CEV). Due to these features, the high strength steel has attracted considerable attention in the construction industry for its use in new structural applications with the help of the appropriate design and fabrication methods. However, due to the lack of sufficient research on the effects of the different post-yield range characteristics of the high strength steel to the structural behavior, the current code directly or indirectly restricts high strength steel by adopting limiting parameters such upper yield strength limit, upper yield-to-tensile (Y/T) strength ratio limit or a certain level of ductility capacity (rotation capacity). The primary target of this research is to experimentally and analytically quantify the effects of the post-yield range characteristics of mild and high strength steel on I-shaped flexural members. In addition, this study attempts to establish a methodology to provide adequate slenderness ratios to ensure inelastic lateral torsional buckling (LTB) strength and a certain level of rotation capacity, related to the existing AISC-LRFD specification and EC 3 code.
This work consists of four major sections: stress-strain curve idealizations, estimation of in-plane rotation capacities, and analytical and experimental studies of inelastic LTB behaviors.
In the stress-strain curve idealizations, tensile coupons of HSA800, SM570, and SM490 plates are tested and statistical regression curves were proposed to predict the Y/T strength ratio and tensile-to-yield (T/Y) strain ratio according to yield strength, which are pivotal values to idealize the initial portion of the stress-strain curve up to tensile strength. Four idealized material models (the traditional model (#1) and the Haaijer model (#2) for mild steelthe Ramberg-Osgood model (#3) for high strength steeland the Piecewise linear model (#4) for both steel grades) with properly assumed parameter values are suggested and numerically verified with the tensile coupon data.
In the estimation of in-plane rotation capacities, a simplified method is proposed to calculate the in-plane rotation capacity at maximum moment of HSA800, SM570, and SM490 I-shaped members under uniform and moment gradient loading conditions by adopting the piecewise linear models. Under uniform moment loading condition, the in-plane rotation capacity is directly proportional to the T/Y strain ratio. On the other hand, at the moment gradient loading condition, three parameters including Y/T strength ratio, T/Y strain ratio, and yield plateau length together influence on the in-plane rotation capacity. Due to high Y/T strength ratio and low T/Y strain ratio of HSA800, the in-plane rotation capacity of HSA800 I-shaped member is inevitably low as compared to other grades (SM570 and SM490) of steel under moment gradient loading condition. Parametric studies were conducted to increase the rotation capacity level of the HSA800 I-shaped member under the moment gradient condition, demonstrating that lowering the Y/T strength ratio to 0.80 levels only does not ensure the satisfactory rotation capacity of the existing AISC-LRFD specification assumedthe increase of T/Y strain ratios is thus inevitably required.
In the analytical studies of inelastic LTB behaviors, the methods to quantify the inelastic section stiffness (effective flexural, warping, and torsional rigidities of I-shaped member fabricated from mild and high strength steel), including the presence of the residual stresses, are proposed by applying the tangent modulus theories. This inelastic section stiffness is crucial to develop the LTB strength and rotation capacity curves of the I-shaped member under uniform and moment gradient loadings. After verifications of the derived strength and rotation capacity curves in current studies with the previous experimental data, parametric studies are conducted to evaluate the geometrical and material effects on the LTB capacity of I-shaped member. By comparing the results of the parametric models with the existing unbraced length limits specified in AISC-LRFD specifications, a methodology to design appropriate I-section geometry depending on the material selection of I-shaped member is proposed.
In the experimental studies, three types of welded I-shaped specimens (type A-[G:H-250x150x15x15]-[M:Ho-775], type B-[G:H-400x150x15x15]-[M:Ho-775], and type C-[G:H-400x150x15x15]-[M:Hy-349-822], where [G:] indicates the cross section geometry[M:Ho] and [M:Hy] indicates the homogeneous and hybrid I-section respectively) were fabricated and tested under uniform moment to examine the geometrical and material effects of the I-section on LTB behaviors. All specimens failed by LTB, triggering a sinusoidal shape failure mode. The measured critical buckling strength and rotation capacity of both type A and type C specimens, where the effective section rigidities to plastic moment ratio are relatively high, satisfy the existing AISC-LRFD specification and EC 3 code. However, type B specimens, where a high height-to-width ratio is applied or the effective section rigidities to plastic moment ratio are relatively low, the current AISC-LRFD unbraced length limit would not give conservative rotation capacity values. By comparing the experimental data with the analytically developed buckling curves, it is shown that the curves well predict experimental LTB strength and rotation capacity values.Chapter 1. Introduction
1.1 Background
1.1.1 Production and mechanical properties of high strength steel
1.1.2 Specified limitation on high strength steels in building codes
1.2 Brief review of influence of post-yield range properties on member behavior
1.2.1 Post-yield range properties
1.2.2 In-plane behavior
1.2.3 Out-of-plane behavior
1.3 Limitation of recent studies and object of this study
1.3.1 Limitation of traditional stress-strain model to apply in high strength steel
1.3.2 Limitation of up-to-date theoretical and experimental researches
1.3.3 Objective of this study
1.4 Scope of work
1.4.1 Background
1.4.2 Development of analytical LTB model for I-shaped members
1.4.3 Development of LTB strength curve for homogeneous I-shaped member
1.4.4 Development of available rotation capacity curve for homogeneous I-shaped member
1.4.5 Development of LTB strength and rotation capacity curves for hybrid I-shaped member
1.5 Methodology
1.5.1 Experimental work
1.5.2 Theoretical work
1.6 Relevance of current studies
1.7 Summary
Chapter 2. Previous Researches
2.1 Introduction
2.1.1 Major buckling phenomenon and the significance of uncoupling approach
2.1.2 Rotation capacity under uniform moment and moment gradient
2.2 Experimental studies of inelastic LTB behavior
2.2.1 Rotation capacity of I-beam under uniform moment
2.2.2 Rotation capacity of I-beam under moment gradient
2.3 Analytical studies of inelastic LTB behavior
2.3.1 I-Beams under uniform moment
2.3.2 I-Beams under moment gradient
2.4. Summary
Chapter 3. Idealized Material Models and In-plane Rotation Capacity
3.1 Characteristics of stress-strain curves
3.1.1 Y/T strength ratio according to yield strength
3.1.2 T/Y strain ratio according to yield strength
3.2 Idealized material models
3.2.1 Traditional model
3.2.2 Haaijer model
3.2.3 Ramberg-Osgood model
3.2.4 Piecewise-linear model (Tri-linear, Bi-linear)
3.3 In-plane rotation capacity
3.3.1 Overview and assumption
3.3.2 In-plane rotation capacity at member maximum moment
3.4 Summary
Chapter 4. Analytical Studies of Inelastic LTB Behaviors
4.1 Derivation of inelastic section rigidities for analyzing inelastic buckling
4.1.1 Tangent modulus theory and its application
4.1.2 Inelastic section rigidities in ideal I-section
4.1.3 Residual stress in I-section
4.1.4 Effects of residual stresses on inelastic section rigidities of I-beam
4.1.5 Summary
4.2 LTB strength under uniform moment
4.2.1 Overview of LTB under uniform moment
4.2.2 Analytical parametric studies
4.2.3 Detailed approach to derive unbraced length limit for achieving plastic moment
4.2.4 Simplified approach to derive unbraced length limit for achieving plastic moment
4.2.5 Summary
4.3 Available rotation capacities (governed by LTB) under uniform moment
4.3.1 Description of the behavior
4.3.2 Derivation of rotation capacity curve under uniform moment via inelastic section rigidities
4.3.3 Validation of the analytically developed rotation capacity curve with previous experiments
4.3.4 Analytical parameter studies
4.3.5 Detailed approach to derive unbraced length limit for target rotation capacity
4.3.6 Simplified approach to derive unbraced length limit for target rotation capacity
4.3.7 Summary
4.4 LTB strength under moment gradient
4.4.1 Overview of LTB under moment gradient
4.4.2 Simplified T-column approach to derive unbraced length limit for achieving plastic moment
4.4.3 Summary
4.5 Available rotation capacitys under moment gradient
4.5.1 Description of the behavior
4.5.2 Derivation of rotation capacity curve under moment gradient via inelastic section rigidities
4.5.3 Simplified T-column approach to derive unbraced length limit for target rotation capacity
4.5.4 Summary
Chapter 5. Experimental Buckling Studies
5.1 Overview of the experimental study
5.1.1 Mechanical properties
5.1.2 Instrumentation plan for measurement
5.1.3 Data processing method
5.1.4 Description of test parameter
5.2 Experimental test results
5.2.1 Specimen Type A: [G:H-250x150x15x15]-[M:H0-775]
5.2.2 Specimen Type B: [G:H-400x150x15x15]-[M:H0-775]
5.2.3 Specimen Type C: [G:H-350x150x30x25]-[M:Hy-349-827]
5.3 Evaluation of the experimental results
5.3.1 Comparison with the code prediction
5.3.2 Comparison with the previous experiments
5.3.3 Comparison with the analytically developed buckling curves
5.4 Summary
Chapter 6. Conclusions
ReferencesDocto
๋ค์ํ ์์ข ์์ ๋ฉํธํ ๋ณ์ด ์ ๋์ ์ข ์ ๋ฉด์ญ์์ฑ ์ฌ์ด ์๊ด๊ด๊ณ์ ๊ดํ ์ฐ๊ตฌ
ํ์๋
ผ๋ฌธ(์์ฌ)--์์ธ๋ํ๊ต ๋ํ์ :์๊ณผ๋ํ ์ํ๊ณผ,2020. 2. ๊น๋์.While genomic alterations in tumors, such as somatic mutations or somatic chromosomal instability, have been reported as reliable biomarkers in immune-oncology, associations between the methylation landscape and tumor immunogenicity is unknown. I sought to find biomarker related to methylation to represent tumor immunogenicity.
I used The Cancer Genome Atlas (TCGA) pan-cancer database (N~8,000) to define methylation burden (MetB) as the number of hypermethylated or hypomethylated CpG sites to represent the degree of aberrant methylation. I comprehensively investigated the association of MetB with cytolytic activity score, calculated by mean of GZMA and PRF1 expression levels, and other various genomic profiles.
The degree of methylation aberrancy correlated with methylation subtypes defined in previous literatures. It also showed negative correlation expression of molecules coordinating immune recognition of tumors. The pan-cancer analysis showed that MetB was negatively correlated with cytolytic activity score (ฯ = -0.37, p < 0.001), independent of mutation burden and chromosomal instability. The negative correlation was consistent in the external cohort of lung adenocarcinoma and low grade glioma (Spearman ฯ = -0.41, p < 0.001 and ฯ = -0.34, p = 0.014, respectively). MetB also had negative correlation with interferon-gamma signatures and was lower in highly immunogenic subtypes of immune landscape. Furthermore, patients with bottom 20% MetB showed longer progression free survival to ipilimumab in TCGA melanoma patients (p = 0.029).
These findings emphasize the importance of methylation aberrancy for tumors to evade immune surveillance and warrant further development of methylation biomarker.์ฒด์ธํฌ ๋์ฐ๋ณ์ด ๋๋ ์ฒด์ธํฌ ์ผ์์ฒด ๋ถ์์ ์ฑ๊ณผ ๊ฐ์ ์ข
์์์์ ์ ์ ์ ๋ณ์ด๊ฐ ์ข
์๋ฉด์ญ์น๋ฃ์์ ์ ๋ขฐํ ์ ์๋ ๋ฐ์ด์ค๋ง์ปค๋ก ๋ณด๊ณ ๋์ด ์์ง๋ง, ์ ์ ์ ๋ฉํธํ์ ๋ณํ์ ์ข
์ ๋ฉด์ญ์์ฑ ์ฌ์ด์ ์ฐ๊ด์ฑ์ ์๋ ค์ ธ ์์ง ์๋ค. ๋ณธ ์ฐ๊ตฌ์์๋ ์ข
์ ๋ฉด์ญ์์ฑ์ ๋ํ๋ด๋ ๋ฉํธํ์ ๊ด๋ จ๋ ๋ฐ์ด์ค๋ง์ปค๋ฅผ ์ฐพ๊ณ ์ ํ๋ค.
TCGA (The Cancer Genome Atlas)์ ์ฝ 8000์ฌ๊ฐ์ ๋ฌํ๋ ์ ์ฒด ์์ข
๋ฐ์ดํฐ๋ฒ ์ด์ค๋ฅผ ํ์ฉํ์ฌ, ๋ฉํธํ ๋ณ์ด ์ ๋๋ฅผ ๊ฒ์ฒด๊ฐ ๊ฐ์ง๊ณ ์๋ ๊ณผ ๋ฉํธํ ํน์ ์ ๋ฉํธํ ๋ CpG ๋ถ์์ ์๋ก ์ ์ํ์๋ค. ์ด๋ ๊ฒ ์ ์๋ ๋ฉํธํ ๋ณ์ด ์ ๋์ GZMA์ PRF1 ์ ์ ์์ ๋ฐํ์ ํ๊ท ๊ฐ์ธ ์ธํฌ ์ฉํดํ์ฑ๋๋ฅผ ๋น๋กฏํ์ฌ ๋ค์ํ ์ข
์ ๋ฉด์ญ์์ฑ๊ณผ์ ์ฐ๊ด์ฑ์ ํฌ๊ด์ ์ผ๋ก ์กฐ์ฌํ์๋ค.
๋ฉํธํ ๋ณ์ด ์ ๋๋ ๊ธฐ์กด์ ๋ฌธํ์ ์ ์๋์๋ ๋ฉํธํ ๋ถ๋ฅ์ ๊ด๋ จ์ฑ์ด ์์๋ค. ๋ํ, ์ข
์ ๋ฉด์ญ ์ธ์์ ๊ด์ฌํ๋ ๋ถ์์ ๋ฐํ๊ณผ ์์ ์๊ด๊ด๊ณ๊ฐ ์๋ ๊ฒ๋ ํ์ธํ์๋ค. ์ ์ฒด ์์ข
๋ถ์์ ํ์์ ๋, ๋ฉํธํ ๋ณ์ด ์ ๋๋ ์ธํฌ ์ฉํดํ์ฑ๋์ ์์ ์๊ด ๊ด๊ณ(ฯ = -0.37, p <0.001)๊ฐ ์์์ ํ์ธํ์๊ณ , ์ด๋ ์ฒด์ธํฌ ๋์ฐ๋ณ์ด ๊ฐ์ ๋ฐ ์ผ์์ฒด ๋ถ์์ ์ฑ๊ณผ ๋
๋ฆฝ์ ์ผ๋ก ์ฐ๊ด์ด ์์์ ํ์ธํ์๋ค. ์ด๋ฌํ ์์ ์๊ด ๊ด๊ณ๋ TCGA ์ด์ธ์ ํ์ ์์ข
๋ฐ ์ ๋ฑ๊ธ ๋๊ต์ข
์ผ๋ก ๊ฐ๊ฐ ๊ตฌ์ฑ๋ ์ธ๋ถ ์ฝํธํธ์์๋ ํ์ธ๋์๋ค (ฯ = -0.41, p <0.001 ๋ฐ ฯ = -0.34, p = 0.014). ๋ฉํธํ ๋ณ์ด ์ ๋๋ ๋ํ ์ธํฐํ๋ก ๊ฐ๋ง ์ ์ ์ ์๊ทธ๋์ฒ์ ์์ ์๊ด๊ด๊ณ๋ฅผ ๋ณด์์ผ๋ฉฐ, ๋ฉด์ญ์์ฑ์ด ๋์ ์ํ์์ ๋ ๋ฎ์ ๊ฒ์ด ํ์ธ๋์๋ค. ๋ํ, TCGA ํ์์ข
ํ์ ์ค ์ดํ๋ฆฌ๋ฌด๋ง ๋ฉด์ญ์น๋ฃ๋ฅผ ๋ฐ์ ํ์๋ค์ ๋์์ผ๋ก ๋ณด์์ ๋, ํ์ 20%์ ๋ฉํธํ ๋ณ์ด๋ฅผ ๊ฐ๋ ํ์๋ค์์ ๋ ๊ธด ๋ฌด์ง๋ณ์งํ์์กด์ ๋ณด์๋ค (p = 0.029). ๊ทธ๋ฆฌ๊ณ ๋ฉด์ญ ๋ฐ์๊ณผ ๊ด๋ จ๋ ์ ์ ์ ํ๋ก๋ชจํฐ์ ๊ณผ ๋ฉํธํ ๋ฐ ์ ๋ฉํธํ๋ ์ธํฌ ์ฉํดํ์ฑ์ ์์ ์ ์ํ๊ฒ ์ํฅ์ ๋ฏธ์ณค๋ค.
์ด๋ฌํ ๊ฒฐ๊ณผ๋ ์ข
์์ ๋ฉํธํ ๋ณ์ด ์ ๋๊ฐ ์ข
์์ ๋ฉด์ญ ํํผ์ ์ค์ํ๋ค๋ ๊ฒ์ ๊ฐ์กฐํ๋ฉฐ, ์ฐจํ ์ด์ ๊ด๋ จ๋ ๋ฐ์ด์ค๋ง์ปค์ ๊ฐ๋ฐ์ด ํ์ํจ์ ์์ฌํ๋ค.Abstract 1
List of Figures 5
List of Tables 7
Introduction 8
Results 10
Defining the degree of methylation aberrancy and its correlation with methylation subtypes 10
Hypermethylation in promoter of CD274 (PD-L1) and human leukocyte antigen correlates decreased corresponding RNA expression 14
Negative correlation of methylation burden with immunogenicity in the tumor microenvironment 21
Methylation aberration in addition to mutation burden and copy number alterations predicting immunogenicity 36
Selection of CpG sites to assess potential of methylation aberrancy as a biomarker 39
Discussion 41
Conclusion 44
Methods 45
Dataset acquisition 45
Determining ฮฒ-score cutoffs and definition of methylation burden 46
Promoter methylation status and expression determination 47
Genomic profile definition 47
Selection of CpG sites 48
Statistical analysis 48
References 50
์ด๋ก 57Maste
The Influence of Total Body Irradiation of X-rayon The Survival of Homologous Skin Grafts in Rats.
The behavior of the homologous skin grafts in rats
irradiated with sublethal dosis of X-ray was studied.
Wistar albino rats were used as recipients and donors
were Long-Evans hooded rats. The sublethal dosis of
total body irradiation of Xยทray to the normal Wistar rats
was approximately 600r-650 r and 500r was estimated
to be sublethal dosis. The skin homografts of 2.0cm.x
2.0 cm. from hooded donors to untreated Wister recipients
survived for 7 to 10days, on average 8. 5 days,
followed by the typical pattern of the skin homograft
re ection; whereas of the 15sublethally irradiated ani~
mals 12showed prolonged survival (4 to weeks) of the
grafts from hooded donors, which were ultimately
replaced by the host tissue with the chronic rejection
pattern, none of them survived permanently
Effect of Yield Strength on Inelastic Lateral Instability and Rotation Capacity of Continuous Steel Beams
ํ์๋
ผ๋ฌธ(์์ฌ) --์์ธ๋ํ๊ต ๋ํ์ :๊ฑด์ถํ๊ณผ,2010.2.Maste