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A Lensball is basically a glass sphere or crystal ball that photographers shoot through to create a fisheye lens look, but for about a fraction of the price. By shooting through the glass ball it becomes a natural frame for your subject.
Refraction happens when light passes through an object of denser mass, as the light passes through, it becomes bent. This is why Lensballs or a crystal ball works so well at refraction. They are made from high quality glass that easily lets light pass through and keeps your image sharp and in focus.
You may not know it, but you are already a refraction photographer. To prove this, simply take off the lens front and rear caps. Look through your lens and you will see the image is upside down and projected through the concave glass just like crystal ball photography.
Some genius rebranded a crystal ball for photographers and the rest is history. You can buy either and capture these types of shots and scenes. When it comes to the world of camera lenses, lens balls and crystal balls are just much cheaper versions of wide angle and fisheye lenses. Lensball range from 20 dollars to 100 where camera lenses can be up in the 1000s.
Results vary based on the size of your Lensball and how far you are from the scene, but you will want to focus your camera on the center of the ball. Remember your image will be upside down inside the ball but this can be fixed later in editing software or with the techniques below.
Take your time! Remember, your ball is made out of glass, so it can easily break. Make sure you place it somewhere steady before shooting, even a little wind can easily knock the ball over and could crack or scratch your new investment.
2. Take your Lensball close to your favorite local landscape. The best way to keep your Lensball in place when working on a hilly surface is to place it in a crack in the street or hold it yourself for your photo.
Refractique: Offers a variety of photography tips and boasts some of the best Lensballs in the world. They offer flawless scratch-free, ultra-polished crystal balls that are designed in the US. The result is flawless shots. All their balls come with a starter guide to show you the technique way to your best images.
Pinterest: This is a great place to get started if you are looking for image ideas. Pinterest is flooded daily with all types of crystal ball photography and will open your mind to all sorts of new possibilities.
To probe the influence of trace surface elemental rearrangement on chemical and physical functions, we sought a novel analysis tool with high elemental sensitivity. X-ray fluorescence microscopy (XFM) provides unparalleled sensitivity for trace element distribution measurements in many micrometer-thick specimens (true microscale battery particles) and facilitates significantly improved sensitivity relative to electron probes35. With X-ray ptychrography, an emerging method that images ultrastructures at beyond-focus-optic resolution, a combined approach with XFM and ptychography can be employed to study elemental localization within the high-resolution structural context, which aids the elucidation of phase transition mechanisms36,37,38. The fluorescence maps (Mn, Co, Ni) in Fig. 5 indicate homogeneous elemental distributions of Ni, Co, and Mn within the pristine single-crystalline particle, while Mn metal segregation and Ni deficiencies are observed within the single-crystalline particle after 200 cycles7. The phase images given by ptychography reveals the projected electron density distribution of the particle along the X-ray beam direction. For the pristine sample in Fig. 5b, the phase map shows a single intact crystal with several facets, which is consistent with the SEM image of pristine particles (Fig. 1a). However, ptychographic image of the particle after 200 cycles shows inhomogeneous morphology, several example locations indicated by white arrows have lower electron density, which is presumably due to the formation of cracks. In addition, small particles with weak phase (indicated by black arrows in Fig. 5c) were observed around the particles, which come from the electrolyte. In all, the projected phase image of the cycled particle is well consistent with the surface morphology given by SEM (Fig. 5d). To better visualize the internal structures and further directly correlate microstructural changes to electrochemical cycle stability, we performed synchrotron X-ray nanotomography39. Fig. 6a illustrates the 3D microstructure of pristine and 200th cycled single-crystalline NCM. Significant amounts of cracks in single-crystalline particles indicate that the integrity of the original microstructural morphology has been destroyed. Close examination of NCM particles after the 200th cycle reveals multiple microcracks on the particles (indicated by the arrow in Fig. 5), which are gaps between primary particles that arose from inhomogeneous diffusion during the cycling process. Figure 6b reveals the internal structural information of the split sample from the 2D projection images extracted along the Z vertical axis. For cycled samples, present internal cracks and fractures can be attributed to heterogeneous phase transition-induced internal strains during long-term cycling. This is consistent with results obtained from SEM (Fig. 6c, d).
It is well known that the Ni-rich rock-salt phase on the surface caused by cation mixing may inhibit lithium-ion transport, which can trigger surface-phase transformations from layered to rock-salt structures and induce inhomogeneous lithium-ion distribution40,41. We employed diffusion-induced stress models to understand the Electrochem-mechanical degradation mechanism and investigate stress change in single-crystal NCM15. Fig. 6e illustrates the heterogeneous stress distribution caused by the inhomogeneous distribution of lithium-ion concentration in single-crystal NCM particles. Such inhomogeneous lithium distribution may cause mismatched strains, which leads to high-stress concentrations near the phase interface (Fig. 6f, g). As cycles proceed, the particles will be lacerated when the fracture strength is unable to sustain the strains, which quickly induces polarization and plummets cycle performance. This mechanism is schematically illustrated in Fig. 6h. As for untreated NCM single crystals, the Ni-rich rock-salt phase of a single-crystal surface inhibits near-surface lithium-ion transport, which results in heterogeneous chemical particle distribution and causes stress generation. Deep lithium extraction/intercalations and stress release further increase internal strain and the presence of intergranular cracks, which decreases the structural robustness of NCM materials.
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