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CRYSTA NOVA P16 High Speed Polarization Camera

photron_crysta_nova_p16_high_speed_polarization_camera
The Photron Crysta NOVA P16 polarization high speed camera is used to quantify and measure physical stress in transparent and semi-transparent fluids and solids. The Photron Crysta P16 polarization camera system can measure at 16,000 fps in full resolution operation or at 1.1 million fps when runnin ...Read more
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The Photron Crysta NOVA P16 polarization high speed camera is used to quantify and measure physical stress in transparent and semi-transparent fluids and solids. The Photron Crysta P16 polarization camera system can measure at 16,000 fps in full resolution operation or at 1.1 million fps when running at reduced resolution.

The Photron Crysta P16 high-speed polarization camera for the two-dimensional analysis of birefringence measurements, film thickness analysis, and surface roughness inspection, and is a powerful tool to understand phenomena such as birefringence, retardation, stress and impact fracture mechanisms of materials and fluids. This systems employ mechanical or electrical drives as polarization modulators, they require several photo-detection processes to measure polarization. In order to overcome this problem, The Crysta NOVA P16 utilizes a ultra fast high-speed 2D birefringence measurement system with a maximon effective polarization sampling resolution of 512 x 512 pixles as the core device of the system with 16 parallel read out circuits in a matrix in the image sensor, which are connected to each pixel with individual A/D converters.

The image sensors design and fabrication incorporates a pixelated polarizer array which is made from photonic crystal bonded directly to the CMOS sensor, making the optical system in this sensor resistant to vibration. Each polarizer corresponds to each pixel of the image sensor with a one to one ratio. The size of each polarizer and pixel is 20 µm x 20 µm. In the polarizer array, groups of four neighboring polarizers (2 x 2) are set to have differing fast axis orientation at 0°, 45°, 90° and 135° in a clockwise arrangement. One polarization datum can be obtained by calculating detected light intensities from the four pixels of the image sensor. The parallel read-out circuit is arranged in a corresponding matrix.

The electric charges that represent the light intensities accumulated from each pixel are quantized by the multi-channel Analog/Digital converters and are stored in the memory of the camera. Once that is done. the software apply a phase shift analysis process to the stored data to obtain time-serial images of birefringent phase difference.

1024 x 1024 @ 16,000fps

Performance examples:

  • 1,024 x 1,204 pixels @ 16,00 fps
  • 1,024 x 768 pixels @ 20,000 fps
  • 1,024 x 512 pixels @ 30,000fps
  • 640 x 640 pixels @ 36,000 fps
  • 512 x 512 pixels @ 50,000 fps

Polarization operating Wavelength

500-550nm

  • Variable Region of Interest (ROI)
  • Capture 12-bit uncompressed data
  • 20 μm pixels ensure best light sensitivity for demanding high-speed or low light applications
  • Phase lock to IRIG/GPS
  • Rear panel has optional HD-SDI outputs for real-time monitoring during setup, recording and playback
  • Optional remote keypad control with integrated viewfinder
  • 128GB memory option for 5.46 seconds recording at 16,000fps
  • 10-Gigabit Ethernet interface
  • Fast Drive optional storage
128GB
1,100,000 fps
200ns
1Gb/10Gb Ethernet
12-bit
Yes
5.46 sec at 1024 x 1000 @ 16,000fps
Global Electronic Shutter
20

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Understanding the Main Features of Cavitar’s CAVILUX Smart and CAVILUX HF Pulsed Illumination Lasers

 Cavitar CAVILUX HF Pulsed Illumination Laser

Cavitar CAVILUX Smart Pulsed Illumination Laser

 

Wavelength and Spectral Characteristics

The wavelength of illumination plays a crucial role in machine vision systems. Selecting the correct wavelength enhances image contrast and reveals specific features that might otherwise remain invisible.

The CAVILUX's monochromatic light eliminates chromatic aberrations commonly found in white light systems. Moreover, unlike coherent laser sources that produce speckle patterns, CAVILUX's low-coherence design delivers clean, speckle-free illumination while maintaining the benefits of laser light.

Different wavelengths offer distinct advantages in machine vision applications:

  • Infrared illumination (like CAVILUX's 810 nm option) diminishes color effects in monochrome images, enhancing contrast of colored objects and simplifying inspection.
  • Visible red light (640 nm in CAVILUX) provides excellent contrast for many applications where visible illumination is preferred.

Ultimately, the monochromatic nature of laser illumination also allows for efficient filtering of thermal light, enabling clear visualization of extremely hot processes like welding, where traditional lighting is overwhelmed by the process's own emissions.

If visible light is necessary, then CAVILUX Smart 650nm and 300W CAVILUX HF 650nm is the standard products with visiable red illumination. The CAVILUX HF is equipped with a visible laser pointer beam (green light). Color cameras typically have an IR cut filter in front of the sensor which blocks 810 nm. Some cameras allow the removal of that filter and in this case CAVILUX 640nm and 810nm pulsed lasers can be used.

Fiber core diameter

CAVILUX Smart pulsed laser has a fiber core diameter of either 3mm or 5 mm, whereas CAVILUX HF pulse laser has a fiber core diameter of 1.5 mm. This means that CAVILUX HF has 4-11 times higher brightness than CAVILUX Smart. Higher brightness enables the illumination of a smaller area from a certain distance or, alternatively, the illumination of a certain area from a greater distance. CAVILUX Smart 200 W provides a higher brightness than CAVILUX Smart 400W if the illuminated area is smaller than 3 mm.

Motion Blur Reduction: 95% Improvement with Laser

Traditional lighting systems struggle with fast-moving objects, creating blurred images that lack precision. The CAVILUX laser system demonstrated a remarkable 95% reduction in motion blur compared to halogen illumination. This dramatic improvement stems from the laser's ability to generate extremely short pulses that effectively "freeze" motion regardless of camera shutter speed.

Unlike conventional lighting, where motion blur increases proportionally with object velocity, the CAVILUX system maintains image clarity at speeds that overwhelm traditional solutions. The laser pulses can be as brief as 50 nanoseconds, which is approximately 200 times shorter than the fastest exposure times achievable with most industrial cameras. Therefore, even when objects move at exceptional speeds, their positions remain fixed during the illumination period.

Minimum pulse duration

The minimum pulse duration for CAVILUX Smart enabling full output power is ~30 ns. CAVILUX Smart can create pulse durations up to 10 ns but then the output power is lower. The minimum pulse duration for CAVILUX HF at full power is ~100 ns and 50 ns at lower output power. A very short pulse may be needed for removing motion blur when a small and fast-moving object is studied at high magnification. CAVILUX Smart has shorter rise and fall times than CAVILUX HF. Therefore, Smart can generate extremely short pulses (below 100 ns) more accurately than CAVILUX HF.

The CAVILUX system's flexibility in pulse duration settings enabled optimization for different applications—shorter pulses for ultra-high-speed phenomena and slightly longer pulses for applications requiring greater illumination intensity. Indeed, the system demonstrated that in accordance with two-photon absorption principles, shorter pulses required significantly less average optical power to achieve equivalent visibility.

For real-time monitoring applications requiring continuous imaging, the laser's high maximum duty cycle supported frame rates up to several MHz for brief periods, outperforming traditional lighting solutions in both speed and clarity.

 

Maximum duty cycle

Due to the difference in duty cycles CAVILUX Smart laser is typically used together with machine vision cameras and CAVILUX HF laser with high speed cameras. CAVILUX Smart laser may also be compatible with certain ultra high speed cameras, depending on the application and camera with short record buffers.

As an example, if the object doesn’t emit thermal light and 100 ns pulses are sufficient for illuminating the object, CAVILUX Smart laser can provide optimal results up to 10 kHz, independent of the minimum exposure time of the camera.

However, if the object emits thermal light (e.g. arc welding), it is usually important that the laser pulse is of similar duration than the camera exposure time (and that the camera exposure time is properly synchronized with the laser pulse). In such a situation, having a camera of 1 µs minimum exposure time, CAVILUX Smart laser can provide optimal results up to 1 kHz (provided that the synchronization between the camera and the laser can be realized properly). Most likely acceptable results can be achieved also at somewhat higher frame rates (up to a few kHz), but the whole camera exposure time won’t be covered by laser illumination anymore (thus making the effects of thermal light stronger than in an ideal situation).

Applications:

Some examples of high-speed video cameras with short-pulse diode lasers include:

  • Welding 
  • Additive manufacturing
  • High voltage switching circuits
  • Flow visualization
  • Ballistics
  • Impact visualization
  • Shock wave analysis
  • Spray visualization
  • Schlieren
  • Shadowgraphy