• 전기학회논문지
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• 제62권8호
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• pp.1151-1156
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• 2013

In this study, to clearly establish the concept of a geometric modeling I apply for the concept of Pushbroom, limited to two-dimensional radiation Locator to provide a three-dimensional information purposes. Respect to the radiation scanner Pushbroom modeling techniques, geometric modeling method was presented introduced to extract three-dimensional information as long as the rotational component of the Gamma-Ray Linear Pushbroom Stereo System, introduced the two-dimensional and three-dimensional spatial information in the matching relation that can be induced. In addition, the pseudo-inverse matrix by using the conventional least-squares method, GCP(Ground Control Point) to demonstrate compliance by calculating the key parameters. Projection transformation matrix is calculated for obtaining three-dimensional information from two-dimensional information can be used as the primary relationship, and through the application of a radiation image matching technology will make it possible to extract three-dimensional information from two-dimensional X-ray imaging.

• JSTS:Journal of Semiconductor Technology and Science
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• 제2권4호
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• pp.246-252
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• 2002

Two kinds of PZT cantilevers integrated with a piezoresistor have been newly designed, fabricated, and characterized for high speed AFM. In first cantilever, a piezoresistor is used to sense atomic force acting on tip, while in second cantilever, a piezoresistor is integrated to calibrate hysteresis and creep phenomena of the PZT cantilever. The fabricated PZT cantilevers provide high tip displacement of $0.55\mu\textrm{m}/V$ and high resonant frequency of 73 KHz. A new cantilever structure has been designed to prevent electrical coupling between sensor and PZT actuator and the proposed cantilever shows 5 times lower coupling voltage than that of the previous cantilever. The fabricated PZT cantilever shows a crisp scanned image at 1mm/sec, while the conventional piezo-tube scanner shows blurred image even at $180\mu\textrm{m}/sec$. The non-linear properties of the PZT actuator are also well calibrated using the piezoresistive sensor for calibration.

• 치과방사선
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• 제27권1호
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• pp.87-97
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• 1997

The purpose of this study was to evaluate the method for quantitative assessment of bone mass from aluminum-equivalent value of hydroxyapatite by using digital imaging system consisted of Power Macintosh 7200/120, 15-inch color monitor, and GT-9000 scanner with transparency unit. After aluminum-equivalent image made from correlation between aluminum thickness and grey scale, the accuracy of conversion to mass from aluminum-equivalent value was evaluated. Measured bone mass was compared with converted bone mass from aluminum-equivalent value of hydroxyapatite block by correlation formula between aluminum-equivalent value of hydroxyapatite block and hydroxyapatite mass. The results of this study were as follow; 1. Correlation between aluminum thickness and grey level for obtaining aluminum-equivalent image was high positively associated(r²=0.99). Converted masses from aluminum-equivalent value were very similar to measured masses. There was, statistically, no significant difference(P<0.05) between them 2. Correlation between hydroxyapatite aluminum-equivalent and hydroxyapatite mass was shown to linear relation (r²=0.95). 3. Converted masses from aluminum-equivalent value of 3 dry mandible segments were similar to measured masses. The difference between the exposure directions was not significantly different(P<0.05).

• 한국레이저가공학회지
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• 제11권1호
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• pp.32-35
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• 2008

In the remote welding system using $CO_2$ laser, laser beam can be rapidly transferred to a workpiece by moving mirrors of scanner system. So, it makes reducing the cycle time of welding process. We can also use and apply various patterns of weld beads by linear controlled mirrors. But most of the domestic car makers have usually applied use stitch-shaped weld bead. In that case, we don't have the merit of remote welding system efficiently. Therefore, in this paper, we investigated the characteristic of weld strength according to patterns of weld bead on $CO_2$ laser welding. And we also studied the relationship between shape of weld bead and value of tensile load.

• Smart Structures and Systems
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• 제22권2호
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• pp.223-230
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• 2018

This study examines a non-contact laser scanning-based ultrasound system, called an angular scan pulse-echo ultrasonic propagation imager (A-PE-UPI), that uses coincided laser beams for ultrasonic sensing and generation. A laser Doppler vibrometer is used for sensing, while a diode pumped solid state (DPSS) Q-switched laser is used for generation of thermoelastic waves. A high-speed raster scanning of up to 10-kHz is achieved using a galvano-motorized mirror scanner that allows for coincided sensing and for the generation beam to perform two-dimensional scanning without causing any harm to the surface under inspection. This process allows for the visualization of longitudinal wave propagation through-the-thickness. A pulse-echo ultrasonic wave propagation imaging algorithm (PE-UWPI) is used for on-the-fly damage visualization of the structure. The presented system is very effective for high-speed, localized, non-contact, and non-destructive inspection of aerospace structures. The system is tested on an aluminum honeycomb sandwich with disbonds and a carbon fiber-reinforced plastic (CFRP) honeycomb sandwich with a layer overlap. Inspection is performed at a 10-kHz scanning speed that takes 16 seconds to scan a $100{\times}100mm^2$ area with a scan interval of 0.25 mm. Finally, a comparison is presented between angular-scanning and a linear-scanning-based pulse-echo UPI system. The results show that the proposed system can successfully visualize defects in the inspected specimens.

• 제어로봇시스템학회논문지
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• 제13권7호
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• pp.664-670
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• 2007

This study deals with image-based visual servoing for automatic recharging of mobile robot. Because mobile robot must be recharged periodically, it is necessary to detect and move to docking station. Generally, laser scanner is used for detect of position of docking station. CCD Camera is also used for this purpose. In case of using cameras, the position-based visual servoing method is widely used. But position-based visual servoing method requires the accurate calibration and it is hard and complex work. Another method using cameras is image-based visual servoing. Recently, image based visual servoing is widely used for robotic application. But it has a problem that cannot have linear trajectory in the 3-dimensional space. Because of this weak point, image-based visual servoing has a limit for real application. In case of 2-dimensional movement on the plane, it has also similar problem. In order to solve this problem, we point out the main reason of the problem of the resolved rate control method that has been generally used in the image-based visual servoing and we propose an image-based visual servoing method that can reduce the curved trajectory of mobile robot in the cartesian space.

• The Journal of Advanced Prosthodontics
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• 제11권5호
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• pp.271-279
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• 2019

PURPOSE. The newest technologies for digital implant impression (DII) taking are developing rapidly and showing acceptable clinical results. However, scientific literature is lacking data from clinical studies about the accuracy of DII. The aim of this study was to compare digital and conventional dental implant impressions (CII) in a clinical environment. MATERIALS AND METHODS. Twenty-four fixed zirconia restorations supported by 2 implants were fabricated using conventional open-tray impression technique with splinted transfers (CII group) and scan with Trios 3 IOS (3Shape) (DII group). After multiple verification procedures, master models were scanned using laboratory scanner D800 (3Shape). 3D models from conventional and digital workflow were imported to reverse engineering software and superimposed with high resolution 3D CAD models of scan bodies. Distance between center points, angulation, rotation, vertical shift, and surface mismatch of the scan bodies were measured and compared between conventional and digital impressions. RESULTS. Statistically significant differences were found for: a) inter-implant distance, b) rotation, c) vertical shift, and d) surface mismatch differences, comparing DII and CII groups for mesial and distal implant scan bodies ($P{\leq}.05$). CONCLUSION. Recorded linear differences between digital and conventional impressions were of limited clinical significance with two implant-supported restorations.

• 대한방사선치료학회지
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• 제16권2호
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• pp.33-41
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• 2004

목적 : 선형가속기의 정도관리 항목 중 광조사야와 방사선조사야의 일치성 검사는 기존에 필름을 이용하여 측정하였다. 하지만 필름을 이용한 측정은 측정관찰자에 따라 오차가 크게 발생하여 이를 개선하기 위해 BIS(Beam Image System) 영상장치를 이용하여 필름과 조사야 일치성을 비교평가 하고자 하였다. 대상 및 방법 : 선형가속기를 이용하여 필름과 BIS 영상장치에 6, 15MV의 광자선을 조사하여 측정하였다. 조사야는 각각 $50{\times}50,\;100{\times}100,\;200{\times}200mm^2$지었고, 갠트리 각도는 필름을 사용시 $0^{\circ}$에서 측정하였고, BIS 영상장치를 사용시에는 $0^{\circ}$와 $270^{\circ}$에서 측정하였다. 그리고 조사야 일치성 측정은 필름을 사용시 눈금자와 필름 스캐너를 이용하였고, BIS 영상장치에서는 스캔된 광조사야와 방사선조사야의 폭을 X축과 Y축으로 각각 측정하여 그 오차값을 구하였다. 결과 : 필름을 이용한 관찰자의 시각적인 측정에서는 광조사야보다 방사선조사야가 더 크게 측정되었으며, 최대 1.9mm의 오차값을 보였다. 필름 스캐너를 이용한 측정에서도 방사선조사야가 더 크게 측정되었으며, 평균 오차값의 크기는 더 작은 값을 보였다. BIS 영상장치를 이용한 측정에서는 필름 사용시와는 반대로 갠트리 $0^{\circ}$와 $270^{\circ}$에서 광조사야가 방사선조사야보다 더 크게 측정되었고, 최대 0.96mm의 오차값을 보였다. ${\Delta}X$, Y축 모두 허용오차의 범위는 $<{\pm}2mm$로 나타났다. 측정된 평균 ${\Delta}X$, Y 오차값은 시각적인 필름측정, 필름스캐너 측정, BIS 순으로 작게 나타났다. 결론 : 본 연구의 측정결과, 필름을 이용한 시각적인 조사야 일치성 평가시에는 관찰자에 따른 측정오차의 값이 크게 나타날 수 있으므로 정확한 정도관리를 위해서는 세심한 주의로 측정할 것과 필요하다면 다른 영상장치의 도움이나 측정도구의 개발로 정확한 측정이 필요하다 하겠다.

• 구강회복응용과학지
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• 제31권4호
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• pp.316-328
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• 2015

목적: 보관 조건과 석고 주입 시간에 따라 알지네이트 인상체로부터 제작된 모형의 정확성을 알아보고자 하였다. 연구 재료 및 방법: 채득된 알지네이트 인상체는 습도가 유지되는 항습조에 보관하는 것과 진료실 내의 공기 중에 노출되는 상태로 보관 조건을 달리하였다. 보관 조건에 따라 각각 즉시, 채득된 후 10분, 30분, 180분, 360분으로 나누어 보관한 후에 석고 모형을 제작하였다. 제작된 석고 모형을 3D 레이저 스캐너로 삼차원 디지털 모형을 구성하였고 구성된 디지털 모형의 참고점에서 거리를 측정하여 변형률을 비교하였다. 또한 각 실험군의 삼차원 디지털 평균 모형을 제작한 후 중첩을 시행함으로써 표면 변위가 발생한 부위와 크기를 확인하였다. 결과: 인상 채득 즉시 제작한 모형의 변형률이 가장 작게 나타났고, 공기 중에 보관한 인상체보다 항습조에 보관한 인상체의 변형률이 작게 나타났다. 석고 주입 시간이 증가함에 따라서 변형률도 증가하였으며, 석고 주입 시간이 180분을 지나면 보관 조건에 관계없이 대구치 부위에서 변형률과 표면 변위가 증가한다. 결론: 알지네이트 인상체로부터 제작된 모형의 정확성을 위해서는 인상 채득 후, 즉시 모형을 제작해야 한다. 보관이 필요한 경우에는 100% 상대습도가 유지되는 항습조를 이용하고, 보관 시간은 180분을 넘지 않도록 해야 정확한 모형을 얻을 수 있다.

• 핵의학기술
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• 제17권2호
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• pp.10-14
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• 2013

Purpose: Due to developed simultaneous PET/MRI, it has become possible to obtain more anatomical image information better than conventional PET/CT. By the way, in the PET/CT, the linear absorption coefficient is measured by X-ray directly. However in case of PET/MRI, the value is not measured from MRI images directly, but is calculated by dividing as 4 segmentation ${\mu}-map$. Therefore, in this paper, we will evaluate the SUV's difference of attenuation correction PET images from PET/MRI and PET/CT. Materials and Methods: Biograph mCT40 (Siemens, Germany), Biograph mMR were used as a PET/CT, PET/MRI scanner. For a phantom study, we used a solid type $^{68}Ge$ source, and a liquid type $^{18}F$ uniformity phantom. By using VIBE-DIXON sequence of PET/MRI, human anatomical structure was divided into air-lung-fat-soft tissue for attenuation correction coefficient. In case of PET/CT, the hounsfield unit of CT was used. By setting the ROI at five places of each PET phantom images that is corrected attenuation, the maximum SUV was measured, evaluated %diff about PET/CT vs. PET/MRI. In clinical study, the 18 patients who underwent simultaneous PET/CT and PET/MRI was selected and set the ROI at background, lung, liver, brain, muscle, fat, bone from the each attenuation correction PET images, and then evaluated, compared by measuring the maximum SUV. Results: For solid $^{68}Ge$ source, SUV from PET/MRI is measured lower 88.55% compared to PET/CT. In case of liquid $^{18}F$ uniform phantom, SUV of PET/MRI as compared to PET/CT is measured low 70.17%. If the clinical study, the background SUV of PET/MRI is same with PET/CT's and the one of lung was higher 2.51%. However, it is measured lower about 32.50, 40.35, 23.92, 13.92, 5.00% at liver, brain, muscle, fat, femoral head. Conclusion: In the case of a CT image, because there is a linear relationship between 511 keV ${\gamma}-ray$ and linear absorption coefficient of X-ray, it is possible to correct directly the attenuation of 511 keV ${\gamma}-ray$ by creating a ${\mu}$map from the CT image. However, in the case of the MRI, because the MRI signal has no relationship at all with linear absorption coefficient of ${\gamma}-ray$, the anatomical structure of the human body is divided into four segmentations to correct the attenuation of ${\gamma}-rays$. Even a number of protons in a bone is too low to make MRI signal and to localize segmentation of ${\mu}-map$. Therefore, to develope a proper sequence for measuring more accurate attenuation coefficient is indeed necessary in the future PET/MRI.