• Title/Summary/Keyword: 4 probe measurement

Search Result 310, Processing Time 0.026 seconds

Measurement of Sucrose Concentration Using a μFIA Biosensor (μFIA 바이오센서를 이용한 자당 농도 측정)

  • Song D. B.
    • Journal of Biosystems Engineering
    • /
    • v.29 no.6 s.107
    • /
    • pp.553-557
    • /
    • 2004
  • A microdialysis coupled flow injection amperometric $({\mu}FIA)$ biosensor was calibrated to measure the concentration of sucrose using 11 standard samples from 2 ml to 70 ml of sucrose solution. The output of the sensor increased linearly with an increase in the sucrose concentration with an $r^2$ correlation of 0.99. The amperometric biosensor was then applied to measure the sucrose concentration of 4 commercial samples (Orange and Pineapple juices, Pepsi, Sprite) and the results compared with those by HPLC. Around $20\~30\%$ error was observed in sucrose concentration measurements of the samples analyzed. The sensor has potential in rapid measurement once the calibration is done. Potential for on-line sensing is also discussed.

Measurement and Analysis of Electromagnetic field for DC electric railway train (직류철도차량에 대한 자계측정 및 분석)

  • Jang, Dong-Uk;Kim, Min-Cheol;Lee, Chang-Mu;Han, Moon-Seob
    • Proceedings of the KIEE Conference
    • /
    • 2005.07b
    • /
    • pp.1637-1639
    • /
    • 2005
  • The measurement of magnetic field is performed about DC and AC magnetic field in test track of depot. The test point is cap, on the converter/inverter box, on the traction motor, on the APSE and on the line filter, the height of measurement is bottom and 50 cm height. In case of AC magnetic field, the selected specific frequency is measured on the converter/inverter box. The AC magnetic field is checked and analysis through RS-232C and notebook PC. The DC magnetic field is measured by using the Hall Probe, test result is saved and analysis by PXI system. On the line filter, the maximum value is 1.4 mT in case of DC magnetic field and 0.044 mT in case of AC magnetic field at 50 Hz.

  • PDF

Measurement of Hydrogenation Characteristics of Pd Film by Using Electrical Resistivity Measurement Technique (전기저항 측정법을 이용한 Pd박막의 수소화 특성 측정)

  • Cho, Young-Sin;Lee, Ho-Jae;Lee, Jong-Suk
    • Transactions of the Korean hydrogen and new energy society
    • /
    • v.7 no.2
    • /
    • pp.173-180
    • /
    • 1996
  • 4-probe resistivity measurement technique was used to study kinetics of hydrogen absorption-desorption on Pd film($520{\AA}$ thick) at room temperature upto 1 bar. Kinetics data are fitted well to 1st order kinetics equation in ${\alpha}$ and ${\alpha}^{\prime}$ phases. In ${\alpha}+{\alpha}^{\prime}$ phase, absorption kinetics was very complicated, but it could be explained partially with nucleation and growth process. Ln(dR/dt) vs. time plot gives rate constant k value(R is resistance of sample, t is time). k value for absorption is $4^{-6}{\times}10^{-4}/sec$ in ${\alpha}$ phase. k is increasing upto $4^{\times}10^{-2}/sec$ as hydrogen pressure increasing in ${\alpha}^{\prime}$ phase. k is proportional to ln(Pop/Peq), where Peq is equilibrium plateau pressure and Pop is the opposing pressure. In contrast to bulk sample k value was decreasing with increasing number of A-D cycling in ${\alpha}^{\prime}$ phase absorption.

  • PDF

Knock Characteristics and Measurement of Knock Location in a 4-Valve SI Engine (4-Valve SI 엔진의 Knock 특성 및 Knock 발생부위 측정)

  • 이경환;이시훈
    • Transactions of the Korean Society of Automotive Engineers
    • /
    • v.6 no.5
    • /
    • pp.153-161
    • /
    • 1998
  • The knock in a spark ignition engine has been investigated to avoid the damage to the engine and unpleasant feeling caused by the pressure waves propagating across the combustion chamber. Knock intensity and knock onset angle were used as physical parameters to quantify the knock characteristics. The knock intensity is defined as a peak to peak value of the bank pass filtered combustion pressure signal and the knock onset angle is determined as the crank angle at which this signal exceeded the threshold level on each cycle. The cyclic variation of knock in four valve single cylinder engine was investigated with these two parameters. The location of autoignition was also examined by ion probes in the cylinder head gasket and squish region in the combustion chamber. For this measurement, a single cylinder engine was modified to accept the pressure transducer, 18 ion probes in the squish region and 8 ion probes in the specially designed PCB (Printed \ulcornerCircuit Board) cylinder head gasket.

  • PDF

Measurement of Flow and Scalar Distribution at Gas Turbine Inlet Section (가스터빈 입구에서의 유동 및 스칼라 분포 특성)

  • Hong, Sung-Kook;Ireland, Peter;Denman, Paul
    • The KSFM Journal of Fluid Machinery
    • /
    • v.13 no.4
    • /
    • pp.45-50
    • /
    • 2010
  • The goal of paper is to investigate the flow and scalar distribution through the HP Nozzle Guide Vane (NGV) passage. Flow and scalar distribution measurement are conducted by using 5-hole pressure probe and $CO_2$ tracing technique, respectively. Three different experimental cases are considered depending on cooling flow condition. The result shows that the vortical secondary flow patterns are observed clearly and these flow characteristics maintain through the NGV passage regardless of cooling flow injection. Compared to center region, the high axial velocity flow is observed near wall region due to cooling flow injection. Without cooling flow, the $CO_2$ (scalar) distribution becomes to be uniform quickly due to the strong flow mixing phenomenon. However, in cases of cooling flow, scalar distribution is significantly non-uniform.

Total temperature investigation in free & wall jet regions (고속 자유/벽 제트 영역에서의 총온도 특성 고찰)

  • Jung Hyungab;Lee Jangwoo;Yu Mansun;Cho Hyunghee;Hwang Kiyoung;Bae Ju chan
    • Proceedings of the Korean Society of Propulsion Engineers Conference
    • /
    • v.y2005m4
    • /
    • pp.329-333
    • /
    • 2005
  • Total temperature distribution in high speed fee & wall jet regions was investigated using the total temperature probe. For the free jet, the distance of probe from the nozzle exit is changed in the range of 1, 2, 4 and 6 times o nozzle exit diameter. Energy separation phenomenon was observed on shear layer between jet and ambient. In wall jet region, impinging plate was fixed at Z/D=2 and total temperature distribution has been measured for various radial distance($R/D=1.25\sim2.0$). Energy separation phenomenon was found at wall jet boundary and near wall, and was compared with measured adiabatic wall temperature value.

  • PDF

A Newly Designed Contact Profiler for Microstructure (새로운 구조의 접촉식 미세구조 프로필러)

  • Choi, Dong-Jun;Choi, Jai-Seong;Choi, In-Mook;Kim, Soo-Hyun
    • Journal of the Korean Society for Precision Engineering
    • /
    • v.19 no.3
    • /
    • pp.39-45
    • /
    • 2002
  • A simple and low cost stylus profiler made of ferrite cores is developed. The devised profiler consists of a contact probe, a measuring transducer, a signal processing unit, and a motorized stage. The contact probe attached to 4-bar spring maintains sufficient stiffness to protect disturbances. An overlap-area type inductive position sensing system is selected as a measuring transducer, which has high sensitivity, repeatability and linearity. The transducer is composed of coil bundles and ferrite cores which have good electromagnetic characteristics in spite of low cost. The repeatability of the profiler with the proposed inductive sensing system is better than 50nm. Experimental results are shown that the proposed profiler can measure the line or 3D profile of an object with sub-micron features.

Study on the Projectile Velocity Measurement Using Eddy Current Probe (와전류 탐촉자를 이용한 총구 탄속 측정에 관한 연구)

  • Shin, Jungoo;Son, Derac
    • Journal of the Korean Magnetics Society
    • /
    • v.25 no.3
    • /
    • pp.83-86
    • /
    • 2015
  • Nowadays the weapon systems are employed air bursting munition (ABM) as smart programmable 40 mm shells which have been developed in order to hit the target with programmed munition that can be air burst after a set distance in the battlefield. In order to improve the accuracy of such a bursting time, by measuring the speed of the munition from the barrel, weapon systems calculate the exact time of flight to the target and then the time information must be inputted to the munition. In this study, we introduce a device capable of detecting a shot at K4 40 mm automatic grenade. The shot is composed of a rotating copper band to convert linear motion into rotary motion when it passes through the barrel, the steel section is exert the effect of fragment and aluminum section to give fuze information. The aluminum section was used to detect munition using eddy current method. To measure muzzle velocity by means of non-contact method, two eddy current probes separated 10 cm was employed. Time interval between two eddy current probe detection times was used as muzzle velocity. The eddy current probe was fabricated U-shape Mn-Zn ferrite core with enamelled copper wire, and 200 kHz alternating current was used to detect inductance change. Measured muzzle velocity using the developed sensor was compared to the Doppler radar system. The difference was smaller than 1%.

Preparation of Sheet with CNT for EMI Shielding and Its EMI Shielding Property (CNT가 함유된 전자파 차폐흡수시트의 제조 및 전자파 차폐특성)

  • Chae, Seong-Jeong;Cho, Bum-Rae;Hong, Byung-Pyo;Lee, Byoung-Soo;Byun, Hong-Sik
    • Applied Chemistry for Engineering
    • /
    • v.21 no.4
    • /
    • pp.430-434
    • /
    • 2010
  • The sheet for electromagenetic interference (EMI) shielding was prepared with slurry made by the mixture of binder, methyl ethyl ketone, cyclohexanone and metal powder. We tried to enhance the shielding efficiency by adding carbon nanotube (CNT), which has known as highly conducting material. Surface and component analyses were carried out with SEM and EDS, respectively. The electric characteristics and EMI shielding efficiencies were measured with 4-point probe measurement and EMI efficiency measurement equipment. The sheet with 2% CNT addition showed the lowest electrical resistance, $13.13{\Omega}}{\cdot}cm$. It also showed the highest EMI shielding efficiency of 63 dB.

Development of Two-color Radiation Thermometer for Harsh Environments

  • Mohammed, Mohammed Ali Alshaikh;Kim, Ki-Seong
    • Journal of ILASS-Korea
    • /
    • v.21 no.4
    • /
    • pp.184-194
    • /
    • 2016
  • Many industrial processes require reliable temperature measurements in harsh environments with high temperature, dust, humidity, and pressure. However, commercially-available conventional temperature measurement devices are not suitable for use in such conditions. This study thus proposes a reliable, durable two-color radiation thermometer (RT) for harsh environments that was developed by selecting the appropriate components, designing a suitable mechanical structure, and compensating environmental factors such as absorption by particles and gases. The two-color RT has a simple, compactly-designed probe with a well-structured data acquisition system combined with efficient LabVIEW-based code. As a result, the RT can measure the temperature in real time, ranging from 300 to $900^{\circ}C$ in extremely harsh environments, such as that above the burden zone of a blast furnace. The error in the temperature measurements taken with the proposed two-color RT compared to that obtained using K-type thermocouple readouts was within 6.1 to $1.4^{\circ}C$ at a temperature range from 200 to $700^{\circ}C$. The effects of absorption by gases including $CO_2$, CO and $H_2O$ and the scattering by fine particles were calculated to find the transmittance of the two wavelength bands of operation through the path between the measured burden surface and the two-color probe. This method is applied to determine the transmittance of the short and long wavelength bands to be 0.31 and 0.51, respectively. Accordingly, the signals that were measured were corrected, and the true burden surface temperature was calculated. The proposed two-color RT and the correction method can be applied to measure temperatures in harsh environments where light-absorbing gases and scattering particles exist and optical components can be contaminated.