Shielded open-circuited probe for in-situ measurements of soil permittivity in Very high frequency (VHF) and Ultra high frequency (UHF) bands

In this paper, the shielded open-circuited probe operating in the wide frequency range from 75MHz to 2GHz is proposed. The probe is made of an SubMiniature version A (SMA) flange connector. The central rod of the SMA connector emerges from a coaxial transition in the flange and shielded by four rods. The robe design allows us to calculate of the probe reflection coefficient S11 used simple analytical transmission line model (TEM wave mode), the parameters of which were calibrated on a set of substances with a known frequency spectrum of permittivity. The refractive index (RI) and normalized attenuation coefficient (NAC) retrieval technique is based on solving the inverse problem of minimizing the residual norm between measured and calculated frequency spectra of reflection coefficient S11. After calibration, the root-mean-square error (determination coefficient) between the measured and calculated module and phase of the reflection coefficient S11 for the sets of calibration media air, distilled water, butanol, pure ice, water solution with NaCl of salinity of 8.9% do not exceed 0.26dB (0.995) and 0.03 rad (0.999), respectively, in the frequency range from 75MHz to 2GHz. The root-mean-square error (determination coefficient) between the measured RI and NAC spectra for four soil cover samples (variation of the clay fraction from 10.5 g/g to 47.6 g/g) using the proposed probe and a precision coaxial cell not exceeds 0.109 (0.993) and 0.057 (0.986), respectively, in the frequency range from 75 MHz to 2 GHz. As a result, it is experimentally shown that RI и NAC can be measured by the proposed non-precision probe with an error comparable to the precision coaxial cell.

Error determination of hidden flows by hydrostatic weighing in parts obtained by casting

The existing methods for detecting of casting defects and their disadvantages are considered. Hydrostatic weighing method is proposed for detecting of hidden fl aws by comparing the reference and calculated densities of the casting, method for calculating of the error is recommended. The adequacy of theoretical calculations is verifi ed experimentally

DIWATA-2 TARGETING ASSESSMENT AND ATTITUDE ERROR DETERMINATION USING A QUATERNION-BASED TRANSFORMATION SYSTEM

Target pointing assessment of a space-borne satellite is vital to its operations especially on microsatellites that have limited camera field of view and attitude control components like in the case of Diwata-2. In this study, two scientific payloads of the satellite were used: the Enhanced Resolution Camera (ERC) with a field of view (FoV) of 89.8 × 67.5 km and a resolution of 54.6 m; and the High Precision Telescope (HPT) with a FoV of 3.1 × 2.3 km and a resolution of 4.7 m. Errors in pointing especially on a payload with a small field of view like the HPT could mean the satellite missing its target. The target pointing of Diwata-2 is assessed by firstly, computing the differences in the coordinates of the planned target, the center of the actual image taken by the satellite and the projected target from the satellite’s attitude logs. As such, a quaternion-based transformation system is created to simulate the satellite’s local vertical local horizontal system from a given Earth-centered inertial system. Secondly, the differences were then tabulated, and its averages were computed to derived pointing corrections. Applying the algorithm to the satellite’s images shows that there is an average error in pitch and roll of 0.590° and 0.004°, 6.436° and 6.503°, −5.8465° and −6.499° between the set target to the actual image acquired, between the actual image and from attitude logs and between the set target and from the attitude logs, respectively.

A beállítási biztonsági margó nagyságának meghatározása fej-nyak daganatok 2D-2D és 3D képvezérelt intenzitásmodulált sugárkezelése esetén

Introduction: Image-guided intensity-modulated radiation therapy is essential for oncology treatment of head-and-neck cancer patients. Aim: MV-kV and CBCT modalities were compared in case of IGRT treatment for head-and-neck cancer patients. Setup error, setup margin (SM), imaging and evaluation times and imaging doses were analyzed. Method: Eight patients’ elective treatment was evaluated, 66 orthogonal MV-kV images and 66 CBCT series were acquired. Setup error measurement was based on bony manual image registration in three translational directions. Normality test and F-test were performed followed by the comparison with independent-samples T-test (p<0,05). The necessary target volume setup margin was calculated based on Van Herk’s equation. Imaging time and setup error determination time were measured. Imaging doses were estimated based on the literature. Results: No statistically significant difference was found between setup errors determined by MV-kV and CBCT (VRT: 0.5 mm, SD = 1.9 vs. 0.4 mm, SD = 2.1, p = 0.371; LNG: 0.2 mm, SD = 2.2 vs. –0.1 mm, SD = 2.2, p = 0.188; LAT: 0.2 mm, SD = 2.2 vs. 0.3 mm, SD = 2.1, p = 0.41). SM values were: VRT: 2.7 mm vs. 2.5 mm; LNG: 2.1 mm vs. 1.3 mm; LAT: 2.2 mm vs. 2.3 mm. Mean imaging time was 0.65 min (MV-kV) vs. 2.29 min (CBCT). Mean setup error determination time was 2.41 min for both modalities. Estimated imaging doses were 6.88 mGy (MV-kV) vs. 17.2 mGy (CBCT) per fraction. Conclusion: The bony anatomy derived image registration based translational setup error determination results in similar values either by MV-kV or by CBCT. Using 3 mm setup margin in all the directions might be adequate. Imaging time is less by MV-kV, significant difference in imaging doses did not appear. Using CBCT is generally suggested. MV-kV might be an alternative in case of need for shortened imaging time. Orv Hetil. 2018; 159(29): 1193–1200.