117 research outputs found

    ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ прСобразования Π₯Π°Ρ„Π° для контроля диспСрсности Π½Π°ΠΊΠ»Π°Π΄Ρ‹Π²Π°ΡŽΡ‰ΠΈΡ…ΡΡ частиц ΠΈ ΠΈΡ… Π°Π³Π»ΠΎΠΌΠ΅Ρ€Π°Ρ‚ΠΎΠ²

    Get PDF
    The dispersion control of micro- and nanoparticles by their images is of great importance for ensuring the specified properties of the particles themselves and materials based on them. The aim of this article was to consider the possibilities of using the Hough transform for dispersion control of overlapping particles and their agglomerates. Analysis of the application of the Hough transform for overlapping particles and their agglomerates showed the following. The particularities of the conventional implementation lead to the preferred registration of large particles, the shift of the centers of overlapping particles, and the distortion of the size values. To use the Hough transform correctly, fine-tuning of all its parameters is required. To automate this process, the dependences of the number and size of particles recorded in the image on the parameters of the Hough transform was investigated. The studies were carried out on test images with a known number and size of particles. The results showed that when the threshold parameters of the Hough transform change, the number of detected particles stabilizes near their optimal values. When the size range of particles detected by the Hough transform changes, the histogram of the particle size distribution changes. In this case, the optimal width of the range is determined by the most stable extremes of the histogram. The maximum center-to-center distance is set at least half of the optimal range. The configuration algorithm is described and implemented. It implies repeatedly running the Hough transform with different combinations of parameters. The algorithm includes stages of coarse and fine-tuning, which allows to getting closer to the optimal parameters. The efficiency of the algorithm has been confirmed on test and real images. Tests have shown that the errors in determining the size and number of particles of the multi-pass Hough transform are on the same level or exceed these indicators for analog methods.ΠšΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΡŒ диспСрсности ΠΌΠΈΠΊΡ€ΠΎ- ΠΈ наночастиц ΠΏΠΎ изобраТСниям ΠΈΠΌΠ΅Π΅Ρ‚ большоС Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅ для обСспСчСния Π·Π°Π΄Π°Π½Π½Ρ‹Ρ… свойств самих частиц ΠΈ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² Π½Π° ΠΈΡ… основС. ЦСлью Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Ρ‹ являлось исслСдованиС возмоТностСй примСнСния прСобразования Π₯Π°Ρ„Π° для контроля диспСрсности Π½Π°ΠΊΠ»Π°Π΄Ρ‹Π²Π°ΡŽΡ‰ΠΈΡ…ΡΡ частиц ΠΈ ΠΈΡ… Π°Π³Π»ΠΎΠΌΠ΅Ρ€Π°Ρ‚ΠΎΠ². Анализ примСнСния прСобразования Π₯Π°Ρ„Π° для Π½Π°ΠΊΠ»Π°Π΄Ρ‹Π²Π°ΡŽΡ‰ΠΈΡ…ΡΡ частиц ΠΈ ΠΈΡ… Π°Π³Π»ΠΎΠΌΠ΅Ρ€Π°Ρ‚ΠΎΠ² ΠΏΠΎΠΊΠ°Π·Π°Π» ΡΠ»Π΅Π΄ΡƒΡŽΡ‰Π΅Π΅. ΠžΡΠΎΠ±Π΅Π½Π½ΠΎΡΡ‚ΠΈ ΠΊΠΎΠ½Π²Π΅Π½Ρ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠΉ Ρ€Π΅Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ приводят ΠΊ ΠΏΡ€Π΅Π΄ΠΏΠΎΡ‡Ρ‚ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ рСгистрации Π±ΠΎΠ»ΡŒΡˆΠΈΡ… частиц, ΡΠΌΠ΅Ρ‰Π΅Π½ΠΈΡŽ Ρ†Π΅Π½Ρ‚Ρ€ΠΎΠ² ΠΏΠ΅Ρ€Π΅ΠΊΡ€Ρ‹Π²Π°ΡŽΡ‰ΠΈΡ…ΡΡ частиц, искаТСнию Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠ². Для ΠΊΠΎΡ€Ρ€Π΅ΠΊΡ‚Π½ΠΎΠ³ΠΎ использования прСобразования Π₯Π°Ρ„Π° трСбуСтся точная настройка всСх Π΅Π³ΠΎ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ². Для Π°Π²Ρ‚ΠΎΠΌΠ°Ρ‚ΠΈΠ·Π°Ρ†ΠΈΠΈ Ρ‚Π°ΠΊΠΎΠΉ настройки исслСдованы зависимости количСства ΠΈ Ρ€Π°Π·ΠΌΠ΅Ρ€Π° рСгистрируСмых Π½Π° ΠΈΠ·ΠΎΠ±Ρ€Π°ΠΆΠ΅Π½ΠΈΠΈ частиц ΠΎΡ‚ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² прСобразования Π₯Π°Ρ„Π°. ИсслСдования ΠΏΡ€ΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡŒ Π½Π° тСстовых изобраТСниях с извСстным количСством ΠΈ Ρ€Π°Π·ΠΌΠ΅Ρ€Π°ΠΌΠΈ частиц. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΈ ΠΏΠΎΡ€ΠΎΠ³ΠΎΠ²Ρ‹Ρ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² прСобразования Π₯Π°Ρ„Π° число рСгистрируСмых частиц стабилизируСтся Π²Π±Π»ΠΈΠ·ΠΈ ΠΈΡ… ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… Π·Π½Π°Ρ‡Π΅Π½ΠΈΠΉ. ΠŸΡ€ΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΈ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π° Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠ², рСгистрируСмых ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π₯Π°Ρ„Π° частиц измСняСтся гистограмма распрСдСлСния частиц ΠΏΠΎ Ρ€Π°Π·ΠΌΠ΅Ρ€Π°ΠΌ. ΠŸΡ€ΠΈ этом ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Π°Ρ ΡˆΠΈΡ€ΠΈΠ½Π° Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π° опрСдСляСтся ΠΏΠΎ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ устойчивым экстрСмумам гистограммы. МаксимальноС ΠΌΠ΅ΠΆΡ†Π΅Π½Ρ‚Ρ€ΠΎΠ²ΠΎΠ΅ расстояниС устанавливаСтся Π½Π΅ ΠΌΠ΅Π½Π΅Π΅ ΠΏΠΎΠ»ΠΎΠ²ΠΈΠ½Ρ‹ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π°. Описан ΠΈ Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌ настройки, ΠΏΠΎΠ΄Ρ€Π°Π·ΡƒΠΌΠ΅Π²Π°ΡŽΡ‰ΠΈΠΉ ΠΌΠ½ΠΎΠ³ΠΎΠΊΡ€Π°Ρ‚Π½Ρ‹ΠΉ запуск прСобразования Π₯Π°Ρ„Π° с Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹ΠΌΠΈ комбинациями ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ². Алгоритм Π²ΠΊΠ»ΡŽΡ‡Π°Π΅Ρ‚ этапы Π³Ρ€ΡƒΠ±ΠΎΠΉ ΠΈ Ρ‚ΠΎΡ‡Π½ΠΎΠΉ настройки, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰ΠΈΠ΅ Ρ‚ΠΎΡ‡Π½Π΅Π΅ приблизится ΠΊ ΠΎΠΏΡ‚ΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹ΠΌ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌ. Π Π°Π±ΠΎΡ‚ΠΎΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π΅Π½Π° Π½Π° тСстовых ΠΈ Ρ€Π΅Π°Π»ΡŒΠ½Ρ‹Ρ… изобраТСниях. ΠŸΡ€ΠΈ этом ΠΏΠΎΠ³Ρ€Π΅ΡˆΠ½ΠΎΡΡ‚ΠΈ опрСдСлСния Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠ² ΠΈ количСства частиц ΠΌΠ½ΠΎΠ³ΠΎΠΏΡ€ΠΎΡ…ΠΎΠ΄ΠΎΠ²ΠΎΠ³ΠΎ прСобразования Π₯Π°Ρ„Π° находятся Π½Π° ΠΎΠ΄Π½ΠΎΠΌ ΡƒΡ€ΠΎΠ²Π½Π΅ ΠΈΠ»ΠΈ прСвосходят Π΄Π°Π½Π½Ρ‹Π΅ ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»ΠΈ Ρƒ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ²-Π°Π½Π°Π»ΠΎΠ³ΠΎΠ²

    Application of the Hough Transform to Dispersion Control of Overlapping Particles and Their Agglomerates

    Get PDF
    The dispersion control of micro- and nanoparticles by their images is of great importance for ensuring the specified properties of the particles themselves and materials based on them. The aim of this article was to consider the possibilities of using the Hough transform for dispersion control of overlapping particles and their agglomerates. Analysis of the application of the Hough transform for overlapping particles and their agglomerates showed the following. The particularities of the conventional implementation lead to the preferred registration of large particles, the shift of the centers of overlapping particles, and the distortion of the size values. To use the Hough transform correctly, fine-tuning of all its parameters is required. To automate this process, the dependences of the number and size of particles recorded in the image on the parameters of the Hough transform was investigated. The studies were carried out on test images with a known number and size of particles. The results showed that when the threshold parameters of the Hough transform change, the number of detected particles stabilizes near their optimal values. When the size range of particles detected by the Hough transform changes, the histogram of the particle size distribution changes. In this case, the optimal width of the range is determined by the most stable extremes of the histogram. The maximum center-to-center distance is set at least half of the optimal range. The configuration algorithm is described and implemented. It implies repeatedly running the Hough transform with different combinations of parameters. The algorithm includes stages of coarse and fine-tuning, which allows to getting closer to the optimal parameters. The efficiency of the algorithm has been confirmed on test and real images. Tests have shown that the errors in determining the size and number of particles of the multi-pass Hough transform are on the same level or exceed these indicators for analog methods

    Review : Deep learning in electron microscopy

    Get PDF
    Deep learning is transforming most areas of science and technology, including electron microscopy. This review paper offers a practical perspective aimed at developers with limited familiarity. For context, we review popular applications of deep learning in electron microscopy. Following, we discuss hardware and software needed to get started with deep learning and interface with electron microscopes. We then review neural network components, popular architectures, and their optimization. Finally, we discuss future directions of deep learning in electron microscopy

    Engineering Education and Research Using MATLAB

    Get PDF
    MATLAB is a software package used primarily in the field of engineering for signal processing, numerical data analysis, modeling, programming, simulation, and computer graphic visualization. In the last few years, it has become widely accepted as an efficient tool, and, therefore, its use has significantly increased in scientific communities and academic institutions. This book consists of 20 chapters presenting research works using MATLAB tools. Chapters include techniques for programming and developing Graphical User Interfaces (GUIs), dynamic systems, electric machines, signal and image processing, power electronics, mixed signal circuits, genetic programming, digital watermarking, control systems, time-series regression modeling, and artificial neural networks

    Foetal echocardiographic segmentation

    Get PDF
    Congenital heart disease affects just under one percentage of all live births [1]. Those defects that manifest themselves as changes to the cardiac chamber volumes are the motivation for the research presented in this thesis. Blood volume measurements in vivo require delineation of the cardiac chambers and manual tracing of foetal cardiac chambers is very time consuming and operator dependent. This thesis presents a multi region based level set snake deformable model applied in both 2D and 3D which can automatically adapt to some extent towards ultrasound noise such as attenuation, speckle and partial occlusion artefacts. The algorithm presented is named Mumford Shah Sarti Collision Detection (MSSCD). The level set methods presented in this thesis have an optional shape prior term for constraining the segmentation by a template registered to the image in the presence of shadowing and heavy noise. When applied to real data in the absence of the template the MSSCD algorithm is initialised from seed primitives placed at the centre of each cardiac chamber. The voxel statistics inside the chamber is determined before evolution. The MSSCD stops at open boundaries between two chambers as the two approaching level set fronts meet. This has significance when determining volumes for all cardiac compartments since cardiac indices assume that each chamber is treated in isolation. Comparison of the segmentation results from the implemented snakes including a previous level set method in the foetal cardiac literature show that in both 2D and 3D on both real and synthetic data, the MSSCD formulation is better suited to these types of data. All the algorithms tested in this thesis are within 2mm error to manually traced segmentation of the foetal cardiac datasets. This corresponds to less than 10% of the length of a foetal heart. In addition to comparison with manual tracings all the amorphous deformable model segmentations in this thesis are validated using a physical phantom. The volume estimation of the phantom by the MSSCD segmentation is to within 13% of the physically determined volume
    • …
    corecore