CT Centre
A dedicated centre for computed tomography (CT) at Southampton, providing complete support for 3D imaging science, serving Engineering, Biomedical, Environmental and Archaeological Sciences. The centre encompasses five complementary scanning systems supporting a wide range of sample sizes (imaged volumes up to 1.5 x 1 x 1m) and resolution (down to ~200nm). Both academic and industrial consultancy services are provided.
F10025
A dedicated centre for computed tomography (CT) at Southampton, providing complete support for 3D imaging science, serving Engineering, Biomedical, Environmental and Archaeological Sciences. The centre encompasses five complementary scanning systems supporting a wide range of sample sizes (imaged volumes up to 1.5 x 1 x 1m) and resolution (down to ~200nm). Both academic and industrial consultancy services are provided.
A dedicated centre for computed tomography (CT) at Southampton, providing complete support for 3D imaging science, serving Engineering, Biomedical, Environmental and Archaeological Sciences. The centre encompasses five complementary scanning systems supporting a wide range of sample sizes (imaged volumes up to 1.5 x 1 x 1m) and resolution (down to ~200nm). Both academic and industrial consultancy services are provided.
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Mechanical Engineering
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Faculty of Engineering and the Environment
F2
SINCLAIR, IAN
Nikon - HMX: 225kV Microfocus Computed Tomography Scanner
This is a custom Nikon XTEK XTH 225 kVp micro-focus CT system equipped with a robotic sample exchanger (~ 150 mm height limit). It is perfect for relatively small specimens (< 300 mm in height) that can be scanned using a 225 kVp X-Ray source. The source can be configured for high resolution or high flux through a range of different anodes; namely a transmission anode (spot ? 1 ?m, low flux), a standard multi-material reflection anode (spot ? 3 ?m, 'normal' flux) and a rotating anode (spot ? 10?m, x3 -5 flux). A labyrinth at the rear of the system allows routing of cables and pipes that can control and feed in-situ rigs for time-resolved (4D) ?-CT experiments.
E10884
This is a custom Nikon XTEK XTH 225 kVp micro-focus CT system equipped with a robotic sample exchanger (~ 150 mm height limit). It is perfect for relatively small specimens (< 300 mm in height) that can be scanned using a 225 kVp X-Ray source. The source can be configured for high resolution or high flux through a range of different anodes; namely a transmission anode (spot ? 1 ?m, low flux), a standard multi-material reflection anode (spot ? 3 ?m, 'normal' flux) and a rotating anode (spot ? 10?m, x3 -5 flux). A labyrinth at the rear of the system allows routing of cables and pipes that can control and feed in-situ rigs for time-resolved (4D) ?-CT experiments.
This is a custom Nikon XTEK XTH 225 kVp micro-focus CT system equipped with a robotic sample exchanger (~ 150 mm height limit). It is perfect for relatively small specimens (< 300 mm in height) that can be scanned using a 225 kVp X-Ray source. The source can be configured for high resolution or high flux through a range of different anodes; namely a transmission anode (spot ? 1 ?m, low flux), a standard multi-material reflection anode (spot ? 3 ?m, 'normal' flux) and a rotating anode (spot ? 10?m, x3 -5 flux). A labyrinth at the rear of the system allows routing of cables and pipes that can control and feed in-situ rigs for time-resolved (4D) ?-CT experiments.
Zeiss - Xradia 510 Versa: High-resolution computed tomography scanner
This scanner uses a two-stage magnification approach to achieve sub-micron spatial resolution at source to object distance much greater than these allowed in conventional XCT systems. Zeiss?s resolution at a distance, RaaDTM, approach combines the geometric magnification of the X-Ray imaging with a smart system of microscope lenses to further magnify the image. The system is fitted with X0.4, X4, X20, and X40 magnification lens mounted on a barrel mount for rapid change over. This means that the operator can achieve submicron resolution (pixel size ? 70 nm or spatial resolution ? 0.7 ?m) at large working distances, allowing for imaging of larger specimens or small specimens in contained in-situ rings. Importantly, the machine is capable of phase-contrast imaging overcoming an imortant limitations of convectional absorption-based CT imaging; i.e. low or complete absence of contrast for low Z materials. The latter is particular useful for biomedical imaging, CFRP and polymer imaging appl
E10960
This scanner uses a two-stage magnification approach to achieve sub-micron spatial resolution at source to object distance much greater than these allowed in conventional XCT systems. Zeiss?s resolution at a distance, RaaDTM, approach combines the geometric magnification of the X-Ray imaging with a smart system of microscope lenses to further magnify the image. The system is fitted with X0.4, X4, X20, and X40 magnification lens mounted on a barrel mount for rapid change over. This means that the operator can achieve submicron resolution (pixel size ? 70 nm or spatial resolution ? 0.7 ?m) at large working distances, allowing for imaging of larger specimens or small specimens in contained in-situ rings. Importantly, the machine is capable of phase-contrast imaging overcoming an imortant limitations of convectional absorption-based CT imaging; i.e. low or complete absence of contrast for low Z materials. The latter is particular useful for biomedical imaging, CFRP and polymer imaging appl
This scanner uses a two-stage magnification approach to achieve sub-micron spatial resolution at source to object distance much greater than these allowed in conventional XCT systems. Zeiss?s resolution at a distance, RaaDTM, approach combines the geometric magnification of the X-Ray imaging with a smart system of microscope lenses to further magnify the image. The system is fitted with X0.4, X4, X20, and X40 magnification lens mounted on a barrel mount for rapid change over. This means that the operator can achieve submicron resolution (pixel size ? 70 nm or spatial resolution ? 0.7 ?m) at large working distances, allowing for imaging of larger specimens or small specimens in contained in-situ rings. Importantly, the machine is capable of phase-contrast imaging overcoming an imortant limitations of convectional absorption-based CT imaging; i.e. low or complete absence of contrast for low Z materials. The latter is particular useful for biomedical imaging, CFRP and polymer imaging appl