• 제목/요약/키워드: total magnetic field

검색결과 199건 처리시간 0.028초

Dual effect of Low- frequency Electromagnetic Field on Muscle Histopathology of Caspian Sea Cyprinus carpio

  • Samiee, Farzaneh;Samiee, Keivandokht
    • 한국어병학회지
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    • 제30권1호
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    • pp.51-61
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    • 2017
  • The effect of electromagnetic field on aquatic organisms has received little attention. In the current study, the effect of 50Hz electromagnetic field on muscle histopathology of Caspian Sea Cyprinus carpio, a species of economic importance, was investigated. A total of 120 healthy fish were used in this study. They were classified randomly in one of two groups as follows: Control or unexposed EMF group and experimental group with 5 different magnetic field intensities (0.1, 1, 3, 5 and 7mT) at 2 different exposure times including 30 and 60 minutes. Fish in the experimental group were exposed only once. Two weeks after exposure, dorsal muscles sectioned transversely, stained and were examined using a light microscope. Histopathologic assessments showed significant difference between control and EMF exposed groups at both 30 min. (p<0.01) and 60 min. (p<0.001) exposure times. We report for the first time that electromagnetic field in interaction with muscular tissue of Cyprinus carpio exhibits a dual effect which depends on the field intensity, and exposure time. At short exposure time (30 min.), EMF stimulates muscle growth process. At longer exposure time (60 min.), EMF can damage muscle tissue and result in muscle necrosis. More research is required to elucidate precise mechanisms involved in muscle hypertrophy and pathologic changes.

Pulsed (Field) Gradient Spin Echo (PGSE) NMR에 의한 ADS/OTAC 혼합 수용액에서의 콜로이드 회합체의 자가 확산 계수 (Self-Diffusion Coefficients of Colloidal Association Structures in ADS/OTAC Mixed Aqueous Solutions by Pulsed (Field) Gradient Spin Echo-NMR)

  • 김홍운;임경희;김은희;정재준
    • 한국응용과학기술학회지
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    • 제19권4호
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    • pp.339-348
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    • 2002
  • Self-diffusion coefficients of colloidal ass9Ciation structures in the aqueous solutions of anionic ammonium dodecyl sulfate (ADS) and cationic octadecyltrimethylammonium chloride (OTAC) surfactants were measured by pulsed-gradient spin echo NMR. The results were interpreted on the basis of the ADS/OTAC/water phase diagram. Crossing the phase boundaries, significant changes in self diffusion coefficients were observed and well correlated to the phase diagram. For the micelles their apparent radii were obtained from Stokes-Einstein equation. Their values were 15 for the ADS micelles and 54 ${{\AA}}$ for the OTAC micelles, respectively. For vesicles which were formed spontaneously at different relative amounts of the surfactants and total surfactant concentrations, the radius was measured as 50 to 200 nm. This result is in fair agreement with those by TEM and light scattering.

포항방사광가속기 킼커 대출력 펄스전원장치 운전특성 (OPERATING CHARACTERISTICS OF THE PLS INJECTION KICKER MODULATOR)

  • 남상훈;정성훈;고인수
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1998년도 하계학술대회 논문집 E
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    • pp.1800-1802
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    • 1998
  • The Pohang Light Source (PLS) is a third generation 2 GeV synchrotron machine. An injection kicker modulator is positioned in the PLS storage ring tunnel. The kicker modulator is driving four kicker magnets simultaneously. The kicker magnets produce magnetic field to deflect the stored beam orbit in the storage ring closer to the injected beam from the PLS beam transfer line. The injected beam then falls into the storage ring beam dynamic aperture. The current kicker modulator was upgraded and installed on August 1995. Since then, the kicker modulator has shown very reliable and stable performance. The kicker modulator specifications are ${\sim}6.0{\mu}s$ full width, ${\sim}24$ kA peak current, and 10 Hz repetition rate. Output current waveform is a half sinusoid. Two thyratron switches(EEV CX-1536AX) are used in the kicker modulator. Total accumulated thyratron heater run hour is about 15,000 hours as of May 1998. Measurement result of spatial magnetic field distribution in the kicker magnet shows good uniformity.

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고응력장의 해석을 위한 대자율 비등방성 연구 (Interpretation of Palaeostress Using Anisotrophy of Magnetic Susceptibility)

  • 김성욱;김인수;이동호;윤운상;정의진;양홍영;전영길
    • 한국지반공학회:학술대회논문집
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    • 한국지반공학회 2003년도 봄 학술발표회 논문집
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    • pp.369-374
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    • 2003
  • A study of anisotropy of magnetic susceptibility (AMS) have been carried out to understand the tectonic stress field of late Cretaceous-Tertiary strata in Yangsan area. A total of 119 independently oriented core samples were collected from 9 sites throughout the area. The study results show that 5 sites are characterized by load foliation, and 4 sites by tectonic foliation. Load foliations caused by the weight of the overlying strata occur in the central part of the study area. Tectonic foliations created by compressional tectonic force show a regional variation in direction: Direction of compression axes derived from tectonic foliation in the southern part of the study area is approximately WNW-ESE, while it changes into NE-SW northern part of the study area. Such compressional directions are compatible with the lineament directions in each area.

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IMAGING THE RADIO HALO IN THE ABELL 2256 CLUSTER OF GALAXIES

  • KIM K.-T.
    • 천문학회지
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    • 제32권2호
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    • pp.75-82
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    • 1999
  • Diffuse radio emission in Abell 2256 was detected above 3 $\sigma$ with DRAO observations at 1420 MHz. The halo size is $\~13' {\times}10' (\~1h^{-1}_{50}\;Mpc$) in full extent and is elongated along a position angle of about $112^{\circ}$. The total flux density contained in the halo is 30$\pm$10 mJy at 1420 MHz and its spectral index is -2.04$\pm$0.04, showing no evidence for steepening up to 1420 MHz. Using the size estimate, yields a more reliable equipartition magnetic field strength which is $0.34(1 + k)^{2/7}{\mu}G$. In addition, five new radio sources are identified.

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A Model Calculation of Solar Microwave Burst Structure

  • Choi, Yong-Seok
    • 한국우주과학회:학술대회논문집(한국우주과학회보)
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    • 한국우주과학회 1995년도 한국우주과학회보 제4권1호
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    • pp.21-21
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    • 1995
  • The structures of 17GHz microwave burst for bipolar sunspots have investigated. which included the effects of the projected shapes of radio sources as they traverse across the solar disk using a magnetic loop employing a model of solenoid coils. An ensemble of high-energy electrons confined in the loop be assumed. The projected brightnesls distributions of gyrosynchrotron emission in x- and o-modes are computed and converted into total intensity and circular polarization difference at 17GHz for various heliocentric distances using numerical integration of the transfer equation along the line of sight. The results of computations at 17GHz for optical thin case will be presented. and the effects of the orientation of the loop will be discussed in detail, as well as the effect of size, position, Structure, and polarization of the emission. Also the results of the various physical P8lrameters such as the strength of magnetic field. high and low energy cut-off of accelerated electrons. spectral index and density of electrons will be preslmted. After comparing the results of model calculation with observations. we found that the observations can be well explained in terms of a loop model and its projection effect.effect.

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YBCO Bulk 초전도체 교류손실의 주파수 의존성 (Frequency dependence of AC loss in YBCO Bulk superconductor)

  • 예정희;나완수;김찬중;홍계원
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1999년도 하계학술대회 논문집 A
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    • pp.259-261
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    • 1999
  • In this paper, we investigated the frequency dependences of AC loss and the magnetic properties of a superconductor using magnetization method. We used the YBCO bulk superconductor sample which has a square-shaped cross sectional area of $6mm{\times}6mm$. and 43mm-long in axial direction. The applied AC magnetic field was parallel to the direction of sample axis. It is observed that YBCO bulk has the diamagnetic properties. AC loss calculation of YBCO bulk superconductor was performed by evaluating the total area of magnetization traces. We performed two cases of experiments, one for $B_m<B_p$ and the other for $B_m<B_p$. The experiments showed that the AC loss dependences on frequency were different in each mode, as was indicated in other publications.

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열 유입률을 고려한 자계-열계 다목적 위상최적설계 (Multi-objective Topology Optimization of Magneto-Thermal Problem considering Heat Flow Rate)

  • 심호경;왕세명;문희곤
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2007년도 제38회 하계학술대회
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    • pp.138-139
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    • 2007
  • This research provides machine designers with some intuition to consider both, magnetic and heat transfer effects. A topological multi-objective function includes magnetic energy and heat inflow rate to the system, which equals to the total heat dissipation by conduction and convection. For the thermal field regarding the heat inflow, introduced as a reaction force, topology design sensitivity is derived by employing discrete equations. The adjoint variable method is used to avoid numerous sensitivity evaluations. As a numerical example, a C-core design excited by winding current demonstrates the strength of the multi-physical approach.

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다목적위성 삼축자력계로부터 관측된 지구자기장에 관한 연구 (Analysis of Geomagnetic Field measured from KOMPSAT-1 Three-Axis Magnetometer)

  • 김정우;황종선;김성용;이선호;민경덕;김형래
    • 자원환경지질
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    • 제37권4호
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    • pp.401-411
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    • 2004
  • 다목적위성 아리랑 1호(KOMPSAT-1)에 장착된 본체 자세제어용 삼축자력계(TAM) 자료로부터 2000년 6월 19일에서 21일 사이의 지구자기장을 추출하였다 전처리과정으로 관측자료를 지구관성좌표계에서 지구고정좌표계로 변환시킨 후, 이를 다시 구면좌표계로 변환하였고, 지구자기장의 영향이 아닌 위성체 내의 전류에 의한 유도자기장은 자기장의 대칭성을 이용하여 제거하였다. 지구 외적 요인에 의한 자기장의 영향을 제거하기 위해 위성 궤도를 상향 및 하향 두 그룹으로 분류한 후, 2차원 파동수대비법을 이용해 두 그룹 사이에 서로 역으로 대비되는 성분을 제거하였다. 측선 잡음을 제거를 위하여 파동수영역에서 사분면교환법을 도입하였고, 이로부터 삼축자력계 관측값으로부터 최증적인 지구자기장을 추출하였다. TAM 자기장의 검증을 위해 다목적위성과 비슷한 시기에 유사한 고도에서 지구자기장을 전문적으로 측정한 ${\phi}$rsted로부터 유도된 지구자기장 및 IGRF2000모델과 비교한 결과 이들 사이의 상관계수는 각각 0.97과 0.96으로 매우 높게 나타났다. 끝으로 이 연구에서 추출한 지구자기장으로부터 구면조화계수를 degree & order 19까지 계산한 후 이를 IGRF ${\phi}$rsted와 Champ 모델과 비교하였다. 이 연구에 의해 일반적인 지구관측위성의 자세보정용 자력계로부터 degree & order 5까지 신뢰성있는 지구자기장의 추출이 가능함은 밝혀졌고, 이로부터 이 연구의 자료처리과정을 도입하면 지구자기장 전문관측위성이 존재하지 않는 기간은 물론 관측이 존재하지 않는 고도에 대한 지구자기장의 추출이 가능하게 되었고 이로부터 전지구 자기장 모델의 저주파 성분을 향상시킬 수 있음이 밝혀졌다.

구면조화해석(球面調和解析)에 의(依)한 한반도내(韓半島內)의 지구자기장(地球磁氣場)의 분포(分布)에 관(關)한 연구(硏究) (Geomagnetic Field Distribution in the Korean Peninsula by Spherical Harmonic Analysis)

  • 민경덕;이선희
    • 자원환경지질
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    • 제12권2호
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    • pp.95-104
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    • 1979
  • The position of any point on the earth's surface can be. represented in the spherical coordinates by surface spherical harmonics. Since geomagnetic field is a function of position on the earth, it can be also expressed by spherical harmonic analysis as spherical harmonics of trigonometric series of $a_m({\theta})$ cos $m{\phi}$ and $b_m({\theta})$ sin $m{\phi}$. Coefficients of surface spherical harmonics, $a_m({\theta})$ and $b_m({\theta})$, can be drawn from the components of the geomagnetic field, declination and inclination, and vice versa. In this paper, components of geomagnetic field, declination and inclination in the Korean peninsula are obtained by spherical harmonic analysis using the Gauss coefficients calculated from the world-wide magnetic charts of 1960. These components correspond to the values of normal geomagnetic field having no disturbances of subsurface mass, structure, and so on. The vertical and total components offer the zero level for the interpretation of geomagnetic data obtained by magnetic measurement in the Korean peninsula. Using this zero level, magnetic anomaly map is obtained from the data of airborne magnetic. prospecting carried out during 1958 to 1960. The conclusions of this study are as follows; (1) The intensity of horizontal component of normal geomagnetic field in Korean peninsula ranges from $2{\times}10^4$ gammas to $2.45{\times}10^4$ gammas. It decreases about 500 with the increment of $1^{\circ}$ in latitude. Along the same. latitude, it increases 250 gammas with the increment of $1^{\circ}$ in longitude. (2) Intensity of vertical component ranges from $3.85{\times}10^4$ gammas to $5.15{\times}10^4$ gammas. It increases. about 1000 gammas with the increment of $1^{\circ}$ in latitude. Along the same latitude, it decreases. 150~240 gammas with the increment of $1^{\circ}$ in longitude. Decreasing rate is considerably larger in higher latitude than in lower latitude. (3) Total intensity ranges from $4.55{\times}10^4$ gammas to $5.15{\times}10^4$ gammas. It increases 600~700 gammas with the increament of $1^{\circ}$ in latitude. Along the same latitude, it decreases 10~90 gammas. with the increment of $1^{\circ}$ in longitude. Decreasing rate is considerably larger in higher latitude as the case of vertical component. (4) The declination ranges from $-3.8^{\circ}$ to $-11.5^{\circ}$. It increases $0.6^{\circ}$ with the increment of $1^{\circ}$ in latitude. Along the same latutude, it increases $0.6^{\circ}$ with the increment of l O in longitude. Unlike the cases of vertical and total component, the rate of change is considerably larger in lower latitude than in higher latitude. (5) The inclination ranges from $57.8^{\circ}$ to $66.8^{\circ}$. It increases about $1^{\circ}$ with 'the increment of $1^{\circ}$ in latitude Along the same latitude, it dereases $0.4^{\circ}$ with the increment of $1^{\circ}$ in longitude. (6) The Boundaries of 5 anomaly zones classified on the basis of the trend and shape of anomaly curves correspond to the geologic boundaries. (7) The trend of anomaly curves in each anomaly zone is closely related to the geologic structure developed in the corresponding zone. That is, it relates to the fault in the 3rd zone, the intrusion. of granite in the 1st and 5th zones, and mountains in the 2nd and 4th zones.

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