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RISS 인기검색어
- 검색키워드
- 저자 : Goharpey, Fatemeh (검색결과 3 건)
- 무료
- 기관 내 무료
- 유료
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A Novel Ultrasonic Gel Phantom Dosimetry for Evaluation of the Dose Response
Goharpey Neda,Mokhtari-Dizaji Manijhe,Bakhshandeh Mohsen 한국물리학회 2020 THE JOURNAL OF THE KOREAN PHYSICAL SOCIETY Vol.77 No.12
Ultrasonic imaging is able to detect structural changes due to chemical reactions occurring due to ionizing irradiation. The purpose of this study to create a gel phantom dosimeter (developed MAGIC gel), which has ultrasonic properties equivalent to human tissue for readout with ultrasonic imaging. The speed of sound and the attenuation coefficient were determined as a function of the absorbed dose in the range of 0-50 Gy by using this dosimeter. A gel phantom was prepared by adding MAGIC polymer gel proprietary combinations in ultrasonic soft tissue-mimicking gel. Then, the ultrasonic parameters (response) of the samples, including the propagation speed of sound (SOS) and the attenuation coefficient (BUA) were measured in the absorbed dose range of 0-50 Gy in steps 2 Gy. The dose response curve is plotted and a sigmoid function is fitted. Ultrasonic images were recorded to assess the quality of the novel gel phantom. At 24 h post-irradiation, the gel samples were imaged by using a magnetic resonance (MR) scanner. The mean values of the transverse relaxation rates (R2) were taken. The sensitivities of the speed of sound and the attenuation coefficient parameters and the R2 parameter were determined for the soft tissue-mimicking ultrasonic gel phantom. The concentrations of gel phantom, including 14% gelatin, 0.25% graphite, and 2% formaldehyde, with a maximum variation in the speed of sound (21.9 ± 2.3, 20.5 ± 2.1, and 24.3 ± 3.3 m/s) and attenuation coefficient (49.6 ± 9.1, 29.5 ± 5.5, and 47.9 ± 15.4 dB/MHz·m) were selected, respectively. The sensitivities of the speed of sound and the attenuation coefficient parameters and the R2 parameter were determined for the soft tissue-mimicking ultrasonic gel phantom as 1.01 m/s, 2.9 dB/MHz·m, and 0.48 s-1 per Gy and for the MAGIC-f polymer gel as 0.79 m/s, 1.9 dB/MHz·m, and 0.26 s-1 per Gy (R = 0.98), respectively. A significant correlation was found between the MAGIC-f polymer gel and the ultrasonic soft tissue-mimicking gel phantom with the R2 parameter (R = 0.9). Thus, the ultrasonic tissue-mimicking gel phantom can be concluded to be suitable for read-out using ultrasound waves as a free radical polymerization sensor. The cost effectiveness due to the utility of edible gelatin and the formation of breast soft tissue-mimicking ultrasonic images due to the presence of graphite scattering particles are distinctive features of the gel phantom introduced in this study.
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Anomalous Rheological Behavior of Dendritic Nanoparticle/Linear Polymer Nanocomposites
Goldansaz, Hadi,Goharpey, Fatemeh,Afshar-Taromi, Faramarz,Kim, Il,Stadler, Florian J.,van Ruymbeke, Evelyne,Karimkhani, Vahid American Chemical Society 2015 Macromolecules Vol.48 No.10
<P>We investigated the effects of soft dendritic polyethylene (dPE) nanoparticles on the rheological properties of a linear polystyrene (PS) matrix. The viscosity of PS–dPE nanocomposites is found to exhibit nonmonotonic dependence on the dPE concentration. In particular, with the addition of 1% dPE nanoparticles, we already observe more than 1 order of magnitude reduction in viscosity. The minimum viscosity was observed at 5% nanoparticles. At dPE concentrations higher than 5%, nanocomposite viscosity increases by addition of nanoparticles, yet it remains below the viscosity of PS. Addition of nanoparticles not only influences the terminal relaxation times of the nanocomposites but also affects their whole relaxation spectra. The viscosity of PS–dPE nanocomposites at high temperature is found to reversibly evolve with time, which proves the existence of supramolecular interactions between the PS matrix and the nanoparticles. Atomic force microscopy confirms that dPE nanoparticles are well distributed in the PS matrix, though each component of the nanocomposite exhibits its own glass transition. While the origin of viscosity reduction remains unknown, it cannot be attributed to confinement, free volume effect, change of entanglement density, surface slippage, shear banding, or particle induced shear thinning.</P><P><B>Graphic Abstract</B> <IMG SRC='http://pubs.acs.org/appl/literatum/publisher/achs/journals/content/mamobx/2015/mamobx.2015.48.issue-10/acs.macromol.5b00390/production/images/medium/ma-2015-003905_0007.gif'></P><P><A href='http://pubs.acs.org/doi/suppl/10.1021/ma5b00390'>ACS Electronic Supporting Info</A></P>
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