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What is depth of fieldformula
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Shallowdepth of fieldphotography
Canning, J.; Lau, A.; Naqshbandi, M.; Petermann, I.; Crossley, M.J. Measurement of Fluorescence in a Rhodamine-123 Doped Self-Assembled “Giant” Mesostructured Silica Sphere Using a Smartphone as Optical Hardware. Sensors 2011, 11, 7055-7062. https://doi.org/10.3390/s110707055
Abstract: The blue OLED emission from a mobile phone was characterised, revealing a sharp emission band centred at λ = 445 nm with a 3dB bandwidth Δλ ∼ 20 nm. It was used to excite Rhodamine 123 doped within a “giant” mesostructured silica sphere during fabrication through evaporative self-assembly of silica nanoparticles. Fluorescence was able to be detected using a standard optical microscope fitted with a green transmission pass filter and cooled CCD and with 1 ms exposure time demonstrating the potential of mobile platforms as the basis for portable diagnostics in the field. Keywords: biological sensing and sensors; optical diagnostics for medicine; fluorescence; optoelectronics; light-emitting diodes; fluorescence microscopy; nanomaterials; silica; optical instruments; smartphones; mobile platforms
Depth of fieldphotography examples
The sample to be tested is a silica mesostructure sphere shown in Figure 3(a). It was fabricated by evaporative self-assembly of a silica solution containing colloidal silica nanoparticles (40 wt% SiO2), measured by dynamic light scattering to have a size distribution of 20–30 nm [11], in water. A small amount of NH4+ prevents aggregation of the silica nanoparticles in solution. In contrast to surfactant based formation of silica mesostructures, where the evaporation rate was optimised by mixing water with ethanol [3], it was found that when starting with nanoparticles the slower the evaporation the larger the spheres and the less likely the cracking. Therefore, no ethanol is required and the evaporation is carried out more slowly with just water. Drops of 10 μL volume were deposited onto a super hydrophobic surface prepared by treating a silver-coated copper plate with heptadecfluoro-1-decanethiol (HFDT) [12]. Upon evaporation (295 K, 1 atm), aggregation and van der Waals attraction led to spheres being formed—contact angles were measured by a small CMOS camera to be α ∼ 150°. The structures tended to be increasingly distorted in shape with enormous potential energy arising from their formation—a few were observed to explode upon drying. The quality of the super hydrophobic surface was also observed to play an important part in the quality of sphere formed. Along with their distorted shape, many were sensitive to perturbations and readily split into halves. In order to investigate this more closely and the possibility of introducing dopants, the fabrication process was repeated by incorporating Rhodamine 123 laser dye, which has a peak absorption at 505 nm and a laser/fluorescence emission ∼560 nm in the green [13]. Generally it was observed that the organic dye appeared to stabilise the formation of the giant spheres allowing spheres up to 1.5 mm to be fabricated with less splitting than that obtained without the use of the dye. One of the larger, distorted spheres that did split into two halves during handling was used as the test sample.
TW Cronin · 2011 · 148 — We review the current state of knowledge concerning how polarization and polarization patterns are formed in nature, emphasizing linearly polarized light.
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Canning J, Lau A, Naqshbandi M, Petermann I, Crossley MJ. Measurement of Fluorescence in a Rhodamine-123 Doped Self-Assembled “Giant” Mesostructured Silica Sphere Using a Smartphone as Optical Hardware. Sensors. 2011; 11(7):7055-7062. https://doi.org/10.3390/s110707055
It is anticipated that by using custom tailored programs the OLED signal intensity can be raised significantly, bearing in mind potential limits in lifetime performance—pulsed operation will help mitigate these issues. Presently, AMOLEDS have relatively low irradiance (∼10,000 cd/me2), but this is improving. Given that these are state-of-the-art easily addressed OLEDs (and LCDs), rapid modulations should in principle be straightforward to program, allowing fluorescence decay measurements to also be undertaken, further increasing potential specimen discrimination
Depth of fielddefinition microscope
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You’ve purchased a camera, you’re out there taking photos, and you’ve made your way to one of the premier resources for all things photography on the web, so I know you want to learn how to create eye-popping photos! With that in mind, here’s an assignment that will help you take your photo taking skills to the next level…
Depth of field (DOF), simply put, is the portion of your photo that is perfectly in focus. Due to the nature of camera components and the way they interact with light, every photo you take (with some random exceptions we won’t get into) will be impacted by your focal length, the distance to your subject (the object or person you are photographing) and your aperture. There are several mathematical calculations involved in determining exactly what depth of field you can expect, but as my goal is to make this subject a simple and easy to remember as possible, I’m going to forgo those explanations for today. If you have some free time and want to explore this in more depth, I’d recommend checking out an online depth of field calculator.
What is depth of fieldin photography
The optical source used to excite this structure on a combined optical and fluorescence microscope set-up was the android mobile Smartphone (HTC Desire). The sample was placed directly on the large area AMOLED screen. Using a freely downloaded application [9], in addition to the white light of all RGB bands together, each RGB component can be selected—specifically, the Rhodamine 123 fluorescence is excited using the 445 nm band.
Depth of fieldphotography settings
Not only is this an example of “the decisive moment,” it is an example of a larger depth of field. This is achieved by being a bit further from the subject in the photo and by having a smaller aperture opening.
For biodiagnostics, fluorescence remains a key testing method in determining quickly the health status of a sample under test (whether it is from a human, a water ecosystem or so on). Fluorescence demands novel integration of both an excitation source and a detector. Two ways are adopted towards this approach: one is to make a handheld device into which a sample on a disposable slide or microfluidic chip is inserted [5]; the second is to integrate totally the excitation source and detector onto the disposable chip using mass cheap technologies such as those based on inkjet deposition [6].
The size of an image sensor, whether digital or film, affects depth of field in a similar way to a lens aperture. This is because depth of field is a product of both the lens aperture and focal length, plus the sensor size relative to that aperture and focal length.
Here is an example of how distance and focal length can impact your depth of field. The closer you are to your subject, the more likely you are to blur out the foreground and background of your photo. That probability increases as you increase your focal length by zooming in. I was less than two feet from Mr. Bug here (close enough for him to stare back at me) and had my lens extended all the way. Even though my aperture was set to a mid-range value of f6.3, the fore and backgrounds are pretty blurry, helping the eye focus on the subject in the center of the frame.
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Mesostructured silica spheres generally are considered a suitable candidate for a range of chemical delivery applications including fluorophore marker transport and drug treatment when sufficiently small [1]. Both solid and hollow spheres can often be produced chemically through reaction after rapid evaporation of hydrolyzed silicon alkoxide—surfactant solutions [2,3], often in spray form. Here, we report on the fabrication of giant (1.5 mm) mesostructured spheres through slow solvent evaporation from the liquid phase of a solution of prepared silica nanoparticles. A super hydrophobic surface overcame surface inhibition to the shell formation. We also report a novel use of a mobile platform—in this case a Smartphone—as optical hardware to excite fluorescence, demonstrating a new approach to portable diagnostics that potentially overcomes many of the limits of existing methods. For example, hardware and data processing limitations are often used to justify the push to low cost lab-on-a-chip [4] technologies, and other compact, disposable optical based sensor technologies, in order to bring affordable instant diagnostics in remote and isolate regions. There are no other viable alternatives at present.
The successful excitation demonstrates the first time a mobile platform has been used as optical hardware raising the possibility of an entirely new approach to practical sensing and diagnostics, including telecommunications and other signal infrastructure test equipment. Two factors make this possible—the state-of-the-art OLEDs on a low temperature prepared silicon transistor backplane and the open access android platform enabling total software control of the platform and its components. The large area screen of the mobile makes it straight forward to simply place a standard low-cost slide, or microfluidic chip, containing the specimen under test. Further, although we were restricted in use to a good optical microscope and fluorescence imaging camera in these experiments, hardware advances will undoubtedly permit the next generation of mobiles to perform integrated detector functions. For example, the existing CCD camera on many phones is capable of being programmed as a detector, although in most cameras the phone is on the opposite side to the screen (two may be used). Importantly, this technology is accessible to all including those within remote developing regions where mobiles have become an essential tool.
A small, tight, dark lens aperture lets less light into the camera, but because it is smaller, it focuses the light very sharply for a greater depth that extends in front of and behind the actual focus distance.
The mesostructured silica sphere research was funded by two Australian Research Council (ARC) Discovery Projects. The HTC platform and its application to optical sensing were provided by John Canning.
For good measure, here is another example with even greater depth of field. To capture this waterfall, I stood pretty close to the edge and shot alongside it while focusing midway across. Because I had a mid-range focal length and had my aperture opening pretty small, all the features in the photo are recognizable. You can clearly see the wall in the background and the rest of the waterfall in the foreground.
From these photos you can clearly see that with minimal effort and a basic understanding of how to control just a single component of your camera, you are able to completely change the texture and appearance of your photos.
Focal length: Greater focal length = shorter DOF. Distance to subject: Greater distance to subject = longer DOF.\ Aperture width: Wider aperture (smaller f number) = shorter DOF.
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Set your camera mode to aperture priority (“A” on Nikon, “Av” on Canon) and work on creating that nice separation from the background. Focus on the ways of doing so that we discussed today.
SEM imaging of other similar spheres shows hexagonal close packing of the nanoparticles. There is, however, a thin porous more “disordered” layer at the surface which may account for the intensified green fluorescence observed there (Figure 4). The interior structure is well ordered by contrast.
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Canning, J.; Lau, A.; Naqshbandi, M.; Petermann, I.; Crossley, M.J. Measurement of Fluorescence in a Rhodamine-123 Doped Self-Assembled “Giant” Mesostructured Silica Sphere Using a Smartphone as Optical Hardware. Sensors 2011, 11, 7055-7062. https://doi.org/10.3390/s110707055
Here is an example of blurred background using my prime lens. Utilizing a lower aperture and getting close to my subject helped keep the face, snow, and ice sharp, but blurred out the background details that may have distracted from the shot.
Canning J, Lau A, Naqshbandi M, Petermann I, Crossley MJ. Measurement of Fluorescence in a Rhodamine-123 Doped Self-Assembled “Giant” Mesostructured Silica Sphere Using a Smartphone as Optical Hardware. Sensors. 2011; 11(7):7055-7062. https://doi.org/10.3390/s110707055
The mobile platform used is the android HTC Desire readily available commercially and which has a relatively large screen area. We chose the android approach purely because it has open source code potentially allowing ready programming of the equipment for specific applications. Figure 1 shows the individual RGB unit OLED components when examined under an optical microscope and camera. Evidently, the length of each component appears adjusted to account for spectral emission variations and average human eye sensitivity variation across RGB. Hence, by individually addressing each OLED its possible to select only the blue, green or red. Some spectral shaping is possible by addressing any combination thereof of these. This ability to individually select each OLED, using available or custom software applications, is part of the inherent power of these Smartphones. When examined with a fitted spectrometer to the microscope, the spectral profiles, shown in Figure 2, are well defined and distinct showing very good RGB contrast, making them suitable as individual fluorescence excitation sources. The blue band is centred at 445 nm and has a 3 dB bandwidth of ∼20 nm, making it suitable for a number of fluorescent markers.
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Today, though, we’re keeping things simple and to the point. To break this somewhat complex interplay between your camera and light down into simpler concepts, remember:
What is depth of fieldin games
Here you can see the dragonfly is in focus, but the grass behind is completely out of focus and blurry. I was close when I snapped this photo and was using my telephoto lens to allow me to get really focused in on my subject. This combination of closeness to the subject and use of a zoom lens enabled this level of background separation even though my aperture was at a mid-range setting.
Canning, J., Lau, A., Naqshbandi, M., Petermann, I., & Crossley, M. J. (2011). Measurement of Fluorescence in a Rhodamine-123 Doped Self-Assembled “Giant” Mesostructured Silica Sphere Using a Smartphone as Optical Hardware. Sensors, 11(7), 7055-7062. https://doi.org/10.3390/s110707055
From this experiment, Rhodamine 123 was successfully integrated into a “giant” silica mesostructure sphere; it appears to be mostly concentrated at the edge of the sphere where the packing density is less uniform and scattering is highest. Based on the number of spheres formed without cracking or exploding during fabrication, the presence of the organic dye near the surface of the spheres helped to stabilise the formation of these spheres, perhaps by reducing the condensation rate and allowing other material to escape. The total integration of dye in silica was ascertained to be low given the relatively long integration time required; although we also note that excitation at 445 nm was on the short wavelength side of the peak absorption at 505 nm. The concentration of dye within the sphere could not be determined and appears to vary between the centre of the sphere and the outer “shell”; regardless, a more suitable fluorescent marker will likely give stronger results.
Canning, J., Lau, A., Naqshbandi, M., Petermann, I., & Crossley, M. J. (2011). Measurement of Fluorescence in a Rhodamine-123 Doped Self-Assembled “Giant” Mesostructured Silica Sphere Using a Smartphone as Optical Hardware. Sensors, 11(7), 7055-7062. https://doi.org/10.3390/s110707055
There are several justifications for the approach proposed here: (1) smart mobile phones commonly used today have state-of-the-art active matrix organic light emitting diode (“AMOLED”) technology, introduced in 2011, driven by a large telecommunications market—as a consequence, this technology has received, and will continue to receive, significant investment ensuring the technology remains leading edge both in terms of the OLED on an amorphous (in some cases polycrystalline) silicon transistor backplane and in terms of the manner in which they can be programmed; (2) mobile platforms are increasingly being considered for signal processing and transmission of sensors which can potentially clip into the device through standard ports [7]; (3) mobile platforms are commonly available in remote regions and villages where, paradoxically, power may not be available for other more essential items. We therefore merge the ideas together and suggest that recent technological developments of mobile platforms (including tablet computers) are making them ideal as universal optical hardware equipment, extending previously proposed ideas for mobiles as software processers or control units for transmitting data or controlling equipment [7,8]. As proof-of-principle we consider the requirement of an excitation source and characterise a standard android platform. The open source platform means it is relatively easily for specific programs to be written to control Google developed Java libraries; in fact, there is already a simple application freely available to control the LED emission profile (by adjusting each OLED type) and intensity [9]. Although in this work we focus on OLED technology, it is clear other competing processes are now equally advanced, including recent liquid crystal display (LCD) technologies on an amorphous silicon backplane [10].
The hemisphere is taken off the super hydrophobic surface and placed onto a glass slide which in turn is placed across the mobile phone screen. Figure 3(a) shows an optical image obtained with the mobile phone using all RGB components. It is approximately 1.5 mm in diameter. A slight reddish tinge is observed from within. Figure 3(b) shows the image when only blue light is emitted—there is no filtering of the light in the microscope. The clear blue optical transmission inside the sphere suggests it is highly uniformly packed with little scattering, in contrast to the edges. In Figure 3(c) a filter (>20 dB contrast) is used to cut out the blue and only allow fluorescing green through. A gain-charged, cooled CCD camera was used to detect the weak signal, where integration was performed over 1 ms. The shell thickness is estimated to be <20 μm.
What isshallowdepth of field
A large, bright lens aperture lets a lot of light into the camera and onto the image sensor, however such a big aperture also results in a very thin plane of focus, and a lot of foreground and/or background blur.
In order to see where depth of field begins to blur the background, look toward the upper right of the photo. There we begin to see the legs and feet of people walking past start to go out of focus. I would have preferred a smaller depth of field but this was a “let me test my manual setting really quick” shot of this boy running past me. I was so focused on getting settings nailed down that I didn’t even notice he’d fallen until I checked my screen and by then he was up and gone!
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Canning, John, Angelica Lau, Masood Naqshbandi, Ingemar Petermann, and Maxwell J. Crossley. 2011. "Measurement of Fluorescence in a Rhodamine-123 Doped Self-Assembled “Giant” Mesostructured Silica Sphere Using a Smartphone as Optical Hardware" Sensors 11, no. 7: 7055-7062. https://doi.org/10.3390/s110707055
Canning, John, Angelica Lau, Masood Naqshbandi, Ingemar Petermann, and Maxwell J. Crossley. 2011. "Measurement of Fluorescence in a Rhodamine-123 Doped Self-Assembled “Giant” Mesostructured Silica Sphere Using a Smartphone as Optical Hardware" Sensors 11, no. 7: 7055-7062. https://doi.org/10.3390/s110707055
© 2011 by the authors; licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution license (http://creativecommons.org/licenses/by/3.0/).
You’ll quickly get the hang of it and be sharing photos that have all your friends praising your photography skills on the social media platform of your choice!