Fluorescence as a phenomenon is part of a larger family of related luminescent processes in which a susceptible substance absorbs light, only to reemit light (photons) from electronically excited states after a given time.
Photo luminescent processes that are generated through excitation, whether this is via physical, mechanical, or chemical mechanisms, can generally be subdivided into fluorescence and phosphorescence. Absorption of a light quantum (blue) causes an electron to move to a higher energy orbit. After residing in this “excited state” for a particular time, the fluorescence lifetime, the electron falls back to its original orbit and the fluorochrome dissipates the excess energy by emitting a photon (green).
Compounds that display fluorescent properties are generally termed fluorescent probes or dyes. Often ‘fluorochrome’ and ‘fluorophore’ are used interchangeably. The term ‘fluorophore’ refers to fluorochromes that are conjugated covalently or through adsorption to biological macromolecules, such as nucleic acids, lipids, or proteins. Fluorochromes come in different flavors and include organic molecules (dyes), inorganic ions (e.g., lanthanide ions such as Eu, Tb, Yb, etc.)fluorescent proteins (e.g., green fluorescent protein) atoms (such as gaseous mercury in glass light tubes).
Recently, inorganic luminescent semiconducting nanoparticles, quantum dots, have been introduced as labels for biological assays, bio-imaging applications, and theragnostic purposes (the combination of diagnostic and therapeutic modalities in one and the same particle).
Fluorescence microscopy provides an efficient and unique approach to study fixed and living cells because of its versatility, specificity, and high sensitivity.
Fluorescence microscopes can both detect the fluorescence emitted from labeled molecules in biological samples as images or photometric data from which intensities and emission spectra can be deduced. By exploiting the characteristics of fluorescence, various techniques have been developed that enable the visualization and analysis of complex dynamic events in cells, organelles, and sub-organelle components within the biological specimen.
The most common techniques are
Fluorescence recovery after photo bleaching (FRAP)
Fluorescence loss in photo bleaching (FLIP)
Fluorescence localization after photo bleaching (FLAP)
Fluorescence resonance energy transfer (FRET)
This presentation is all about chromatography, its types, different techniques of chromatography. Also it contains the principle, method, applications of column chromatography.
This presentation is all about chromatography, its types, different techniques of chromatography. Also it contains the principle, method, applications of column chromatography.
Sepration of molecules on the basis of applied Electric Field
Categorized into 1) Zone Electrophoresis 2) Moving Boundary Electrophoresis
We can seprate macromolecules (DNA , RNA, PROTEINS )on the basis of their charge, size shape & molecular weight
Spectroscopy techniques, it's principle, types and applications NizadSultana
Spectroscopy and it's applications as well as it's types like Infrared spectroscopy and ultraviolet spectroscopy and principle of spectroscopy why we use spectroscopy.
A technique to determine concentration of elements in the solution by aspirating this sample into flame. Evaporation, Atomization, Excitation ,Emission and Ionization occur in the flame.
Sepration of molecules on the basis of applied Electric Field
Categorized into 1) Zone Electrophoresis 2) Moving Boundary Electrophoresis
We can seprate macromolecules (DNA , RNA, PROTEINS )on the basis of their charge, size shape & molecular weight
Spectroscopy techniques, it's principle, types and applications NizadSultana
Spectroscopy and it's applications as well as it's types like Infrared spectroscopy and ultraviolet spectroscopy and principle of spectroscopy why we use spectroscopy.
A technique to determine concentration of elements in the solution by aspirating this sample into flame. Evaporation, Atomization, Excitation ,Emission and Ionization occur in the flame.
Fluorimetry, principle, Concept of singlet,doublet,and triplet electronic sta...Vandana Devesh Sharma
Content-Principle
concept of singlet, doublet and triplet electronic stages,
Internal and external conversions,
Factors affecting fluorescence,
quenching,
Instrumentation and
applications
Types of luminescence including
bioluminescence,
chemiluminescence,
Fluorescence, and
phosphorescence
These various forms of luminescence differ in their method of emitting light.
Bioluminescence
Chemiluminescence
Fluorescence is the emission of light by a substance that has absorbed light or other electromagnetic radiation.
In most cases, the emitted light has a longer wavelength, and therefore a lower photon energy, than the absorbed radiation
In fluorescence, absorption and emission light takes place in very short time (10-12 or 10-9 seconds)
Fluorescence starts immediately after the absorption of light and stops as soon as the incident light is cut off
Eg -The fluorescent clothes, shoes
Fluorescence is the emission of light by a substance that has absorbed light or other electromagnetic radiation.
In most cases, the emitted light has a longer wavelength, and therefore a lower photon energy, than the absorbed radiation
In fluorescence, absorption and emission light takes place in very short time (10-12 or 10-9 seconds)
Fluorescence starts immediately after the absorption of light and stops as soon as the incident light is cut off
Eg -The fluorescent clothes, shoes
Fluorescence is the emission of light by a substance that has absorbed light or other electromagnetic radiation.
In most cases, the emitted light has a longer wavelength, and therefore a lower photon energy, than the absorbed radiation
In fluorescence, absorption and emission light takes place in very short time (10-12 or 10-9 seconds)
Fluorescence starts immediately after the absorption of light and stops as soon as the incident light is cut off
Eg -The fluorescent clothes, shoes
Fluorescence is the emission of light by a substance that has absorbed light or other electromagnetic radiation.
In most cases, the emitted light has a longer wavelength, and therefore a lower photon energy, than the absorbed radiation
In fluorescence, absorption and emission light takes place in very short time (10-12 or 10-9 seconds)
Fluorescence starts immediately after the absorption of light and stops as soon as the incident light is cut off
Eg -The fluorescent clothes, shoes
Fluorescence is the emission of light by a substance that has absorbed light or other electromagnetic radiation.
In most cases, the emitted light has a longer wavelength, and therefore a lower photon energy, than the absorbed radiation
In fluorescence, absorption and emission light takes place in very short time (10-12 or 10-9 seconds) Fluorimetry
An analytical technique for identifying and characterizing minute amounts of substance by excitation of the substance with a beam of ultraviolet/Visible light and detection and measurement of the characteristic wavelength of fluorescent light emitted.Excited – State Processes in molecules
Fluorescence , Phosphorescence and photoluminescencePreeti Choudhary
luminescence, fluorescence and example of fluorescence, phosphorescence , Jablonski diagram, Photoluminescence.
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describes the complete history, mechanisms, instrumentation(jablonski diagram), types, comparision and factors affecting, applications of fluorescence and phosphorescence and describes about quenching and stokes shift.
Introduction, theoretical principle, quantum efficiency of fluorescence, molecular structure of
fluorescence, instrumentation, factors influencing the intensity of fluorescence, comparison of
fluorometry with spectrophotometry, application of fluorometry in pharmaceutical analysis
Spectrofluorimetry or fluorimetry (www.Redicals.com)Goa App
The term fluorescence comes from the mineral fluorspar (calcium fluoride) when Sir George G. Stokes observed in 1852 that fluorspar would give off visible light (fluoresce) when exposed to electromagnetic radiation in the ultraviolet wavelength.
Structure and function of immunoglobulins(antibodies) Likhith KLIKHITHK1
Immunoglobulins (Ig) or antibodies are glycoproteins that are produced by plasma cells. B cells are instructed by specific immunogens.For, example, bacterial proteins, to differentiate into plasma cells, which are protein-making cells that participate in humoral immune responses against bacteria, viruses, fungi, parasites, cellular antigens, chemicals, and synthetic substances.
The immunogen or antigen reacts with a B-cell receptor (BCR) on the cell surface of B lymphocytes, and a signal is produced that directs the activation of transcription factors to stimulate the synthesis of antibodies, which are highly specific for the immunogen that stimulated the B cell. Furthermore, one clone of B cell makes an immunoglobulin (specificity). Besides, the immune system remembers the antigens that caused a previous reaction (memory) due to the development of memory B cells. These are intermediate, differentiated B cells with the capability to quickly become plasma cells. Circulating antibodies recognize antigen in tissue fluids and serum. This activity describes the physiology and pathophysiology of immunoglobulins
Quantitative estimation of carbohydrates Likhith KLIKHITHK1
Carbohydrates are one of the three macronutrients in the human diet, along with protein and fat. These molecules contain carbon, hydrogen, and oxygen atoms. Carbohydrates play an important role in the human body. They act as an energy source, help control blood glucose and insulin metabolism, participate in cholesterol and triglyceride metabolism, and help with fermentation. The digestive tract begins to break down carbohydrates into glucose, which is used for energy, upon consumption. Any extra glucose in the bloodstream is stored in the liver and muscle tissue until further energy is needed. Carbohydrates is an umbrella term that encompasses sugar, fruits, vegetables, fibers, and legumes. While there are numerous divisions of carbohydrates, the human diet benefits mostly from a certain subset.
The advent of the polymerase chain reaction (PCR) radically transformed biological science from the time it was first discovered (Mullis, 1990). For the first time, it allowed for specific detection and production of large amounts of DNA. PCR-based strategies have propelled huge scientific endeavors such as the Human Genome Project. The technique is currently widely used by clinicians and researchers to diagnose diseases, clone and sequence genes, and carry out sophisticated quantitative and genomic studies in a rapid and very sensitive manner. One of the most important medical applications of the classical PCR method is the detection of pathogens. In addition, the PCR assay is used in forensic medicine to identify criminals. Because of its widespread use, it is important to understand the basic principles of PCR and how its use can be modified to provide for sophisticated analysis of genes and the genome
Recently, the advantages of biopolymers over conventional plastic polymers are unprecedented, provided that they are used in situations in which they raise the functionality and generate extra benefits for human life. Therefore, biopolymers have received much attention because they play an important place in day-to-day life for their specific tunable characteristics, making them attractive in a wide range of applications. Biopolymers can produce materials with tunable properties such as biodegradability, biocompatibility, renewability, inexpensiveness, availability, which are critically important for designing materials for use in biomedical applications. In addition to these properties, smart biopolymers could be prepared by changing the polymer components, which would create more target oriented applications. Biopolymers are potentially used in biomedical applications, including drug delivery, infections, tissue engineering, wound healings, and other as wells.
Quantitative estimation of protein Likhith KLIKHITHK1
Proteins are polypeptide structures consisting of one or more long chains of amino acid residues. They carry out a wide variety of organism functions, including DNA replication, transporting molecules, catalyzing metabolic reactions, and providing structural support to cells. A protein can be identified based on each level of its structure. Every protein at least contains a primary, secondary, and tertiary structure. Only some proteins have a quaternary structure as well. The primary structure is comprised of a linear chain of amino acids. The secondary structure contains regions of amino acid chains that are stabilized by hydrogen bonds from the polypeptide backbone. These hydrogen bonds create alpha-helix and beta-pleated sheets of the secondary structure. The three-dimensional shape of a protein, its tertiary structure, is determined by the interactions of side chains from the polypeptide backbone. The quaternary structure also influences the three-dimensional shape of the protein and is formed through the side-chain interactions between two or more polypeptides. Each protein at least contains a primary, secondary, and tertiary structure. Only some proteins have a quaternary structure as well.
Accurate protein quantitation is essential to protein studies in a multitude of research topics. A wide array of different methods have been developed to quantitate both complex mixtures of proteins as well as a single type of protein.
Total protein quantitation methods comprise traditional methods such as the measurement of UV absorbance at 280 nm, Bicinchoninic acid (BCA) and Bradford assays, as well as alternative methods like Lowry or novel assays developed by commercial suppliers, which often provide a well-designed, convenient kit for each type of the assay. Individual protein quantitation methods include enzyme-linked immunosorbent assay (ELISA), western blot analysis, and more recently, mass spectrometry, among others. Accurate protein quantitation is essential to all experiments related to proteins studies in a multitude of research topics. Different wide array of different methods have been developed to quantitate both complex mixtures of proteins in a given assay for total protein content and as well as for a single type of protein.
Transparent unstained samples do not absorb light and are called phase objects. When light passes through a sample area with no phase object, there is no significant change in the refractive index or optical path length. Non-diffracted light is referred to as direct or zero-order light as it continues unchanged through the sample. On the other hand, when the light passes through an area of the sample with a phase object, small changes in the refractive index will diffract and scatter some light and cause changes to the optical path length, depending on the thickness and refractive index of each structure. Thicker the structure, the greater the diffraction of the light. The diffracted light represents only a small part of the total light that has passed through the sample. This diffracted light arrives at the detector out of phase with the direct light. The small phase shift created by this, is not enough to cause great interference between the direct and diffracted light. Which along with the low absorption of transparent structures means there is negligible amplitude difference between areas where such structures are present and where they are not. Phase-contrast microscopy is a method that manipulates this property of phase objects to introduce additional interference between the direct and diffracted light. This method transforms differences in phase into differences in brightness, increasing contrast in images of non-absorbing samples.
In light microscopy, illuminating light is passed through the sample as uniformly as possible over the field of view. For thicker samples, where the objective lens does not have sufficient depth of focus, light from sample planes above and below the focal plane will also be detected. The out of focus light will add blur to the image reducing the resolution. In fluorescence microscopy, any dye molecules in the field of view will be stimulated, including those in out-of-focus planes. Confocal microscopy provides a means of rejecting the out-of-focus light from the detector such that it does not contribute blur to the images being collected. This technique allows for high-resolution imaging in thick tissues.
In a confocal microscope, the illumination and detection optics are focused on the same diffraction limited spot in the sample, which is the only spot imaged by the detector during a confocal scan. To generate a complete image, the spot must be moved over the sample and data collected point by point.
A significant advantage of the confocal microscope is the optical sectioning provided, which allows for 3D reconstruction of a sample from high-resolution stacks of images. The primary functions of a confocal microscope are to produce a point source of light and reject out-of-focus light, which provides the ability to image deep into tissues with high resolution, and optical sectioning for 3D reconstructions of imaged samples. The basic principle include illumination and detection optics are focused on the same diffraction-limited spot, which is moved over the sample to build the complete image on the detector. The entire field of view is illuminated during confocal imaging, anything outside the focal plane contributes little to the image, lessening the haze observed in standard light microscopy with thick and highly-scattering samples, and providing optical sectioning.
Atomic force microscope (AFM) is a scanning near-field tool for nanoscale investigation which was invented in 1986. Instead of using light or electron beam, AFM uses a sharp tip to ‘‘feel’’ samples. As the tip radius of curvature is on the order of nanometers, AFM can detect changes at a spatial resolution up to sub nanometer level. Compared to the optical microscope, AFM has a much higher spatial resolution which provides the ability to investigate ultrafine structure of samples and even map the distribution of single molecules.
As AFM utilizes direct contact between the tip and the sample, minimum or even no sample preparation is required.
Moreover, AFM can investigate samples in liquid which provides an opportunity to monitor samples close to their native surroundings. Further, AFM provides true 3D images. With optical and electron microscopies, only limited ranges in heights can be ‘‘in-focus’’ at any one time. Therefore, AFM can provide unique insight into the structure and functional behavior of materials. AFM is a versatile technique. Besides scanning the topography of a sample, it can also be used to investigate the mechanical properties of the sample as well as the interactions between the tip and the sample. AFM has been successfully applied in widespread branches of science and technology such as nanofabrication, material science, chemical and drug engineering, biotechnology and microbiology. As for above mentioned reasons, Atomic force microscope (AFM) is considered a useful tool for the nanoscale measurement in material-polymer science and engineering. AFM lacks the robust ability to chemically characterize materials.
Transmission electron microscope (TEM) Likhith KLIKHITHK1
Microscopy is a means by which an object is transformed in to magnified image. There are different ways for magnifying the images of very small objects by large amounts. In any type of microscopy (optical microscopy or electron microscopy), a wave of wavelength λ (light wave or electron wave) interacts with the matter and as a result of this interaction we get the
microstructural information about the object. As the study of the materials at the nano-metric level is drawing much attention of the researchers in the current era, Electron Microscopy becomes a very important physical characterization tool at the nano-metric level. Electron Microscopy stands far ahead of the optical microscopy as it can provide the much improved
resolution and depth of focus compared to optical microscopy. This is a very introductory report on the basics of the electron microscopy (particularly on Transmission electron microscopy). Transmission electron Microscopy (TEM) operates on the same basic principles as the light microscope but uses electrons as “light source” and their much lower wavelength makes it possible to get a resolution thousand times better than with a light Microscopy.
Scanning electron microscopy (SEM) Likhith KLIKHITHK1
Scanning Electron Microscope functions exactly as their optical counterparts except that they use a focused beam of electrons instead of light to “image” the specimen and gain information as to its structure and composition. Given sufficient light, the unaided human eye can distinguish two points 0.2 mm apart. If the points are closer together, they will appear as a single point. This distance is called the resolving power or resolution of the eye. Similarly, light microscopes use visible light (400- 700nm) and transparent lenses to see objects as small as about one micrometer (one millionth of a meter), such as a red blood cell (7 μm) or a human hair (100 μm). Light microscope has a magnification of about 1000x and enables the eye to resolve objects separated by 200 nm. Electron Microscopes were developed due to the limitations of light microscopes, which are limited by the physics of light. Electron Microscopes are capable of much higher magnifications and have a greater resolving power than a light microscope, allowing it to see much smaller objects at sub cellular, molecular and atomic level. The smallest the wavelength of the illuminating sources is the best resolution of the microscope. De Broglie defined the wavelength of moving particles (electron) λ = h/mv, Where λ= wavelength of particles, h= Planck, s constant, m= mass of the particle (electron), v= velocity of the particles; after substituting the known values, λ = 12.3 Ao/V. The resolution of an optical microscope is defined as the shortest distance between two points on a specimen that can still be distinguished by the observer or camera system as separate entities. Resolution (r) = λ/ (2NA), Where λ is the imaging wavelength, NA is objective numerical aperture. Magnification is the process of enlarging the appearance, not physical size, of something. Magnification is defined as the ratio of image distance versus object distance. M= v/u, Where M= magnification, u= object distance, v= image distance. Magnification is also defined as the ratio of the resolving power of the eye to resolving power (δ) of the microscope M= δ eye/ δ microscope.
Crystallography and X-ray diffraction (XRD) Likhith KLIKHITHK1
Atoms in materials are arranged into crystal structures and microstructures.
Periodic arrangement of atoms depends strongly on external factors such as temperature, pressure, and cooling rate during solidification. Solid elements and their compounds are classified into amorphous, polycrystalline, and single crystalline materials. The amorphous solid materials are isotropic in nature because their atomic arrangements are not regular and possess the same properties in all directions. In contrast, the crystalline materials are anisotropic because their atoms are arranged in regular and repeated pattern, and their properties vary with direction. The polycrystalline materials are combinations of several crystals of varying shapes and sizes. The properties of polycrystalline materials are strongly dependent on distribution of crystals sizes, shapes, and orientations within the individual crystal. Diffraction pattern or intensities of X-ray diffraction techniques are used for characterizing and probing arrangement of atoms in each unit cell, position of atoms, and atomic spacing angles because of comparative wavelength of X-ray to atomic size.The X-ray diffraction, which is a non-destructive technique, has wide range of material analysis including minerals, metals, polymers, ceramics, plastics, semiconductors, and solar cells. The technique also has wide industry application including aerospace, power generation, microelectronics, and several others. The X-ray crystallography remained a complex field of study despite wide industrial applications.
Fourier transform infrared spectroscopy (FTIR) is a largely used technique to identify the functional groups in the materials (gas, liquid, and solid) by using the beam of infrared radiations. An infrared spectroscopy measures the absorption of IR radiation made by each bond in the molecule and as a result gives spectrum which is commonly designated as % transmittance versus wavenumber (cm−1). The IR region is at lower energy and higher wavelength than the UV-visible light and has higher energy or shorter wavelength than the microwave radiations. For the determination of functional groups in a molecule, it must be IR active. An IR active molecule is the one which has dipole moment. When the IR radiation interacts with the covalent bond of the materials having an electric dipole, the molecule absorbs energy, and the bond starts back and forth oscillation. Therefore, the oscillation which cause the change in the net dipole moment of the molecule should absorb IR radiations.
A single atom doesn’t absorb IR radiation as it has no chemical bond.
Symmetrical molecules also do not absorbed IR radiation, because of zero dipole moment. For example, H2 molecule has two H atoms; both cancel the effect of each other and giving zero dipole moment to H2 molecule. Therefore, H2 molecule is not an IR active molecule. On the other hand, HF is an IR active molecule, because when IR radiation interacts with HF molecule, the charge transferred toward the fluorine atom and as a result fluorine becomes partial negative and hydrogen becomes partial positive, giving net dipole moment to H-F molecule. A particular IR radiation will be absorbed by a particular bond in the molecule, because every bond has their particular natural vibrational frequency. For example, a molecule such as acetic acid (CH3COOH) containing various bonds (C-C, C-H, C-O, O-H, and C=O), all these bonds are absorbed at specific wavelength and are not affected by other bond. In general we can say that two molecules with different structures don’t have the same infrared spectrum, although some of the frequencies might be same.
UV-visible spectroscopy is a fast analytical technique that measures the absorbance or transmittance of light. Although the UV wavelength ranges from 100–380 nm and the visible component goes up to 800 nm, most of the spectrophotometers have a working wavelength range between 200–1100 nm.
The practical range for UV-vis spectroscopy varies from 200–800 nm; above 800 nm is infrared, while below 200 nm is known as vacuum UV. The ability of matter to absorb and to emit light is what defines its color and the human eye is capable of differentiating up to 10 million unique colors. Light passes through media (transmission), reflects off both opaque and transparent surfaces, and is refracted by crystals. Covalently unsaturated compounds with electronic transition energy differences equivalent to the energy of the UV-visible light absorb at specific wavelengths. These compounds are known as chromophores and are responsible for their color. Covalently saturated groups that do not absorb UV-visible electromagnetic radiation but affect the absorption of chromophore groups are called auxochromes. When UV-vis radiation hits chromophores, electrons in the ground state jump to an excited state, which we refer to as electron-excitation, while auxochromes are electron-donating and have the capacity to affect the color of choromophores while they do not change color themselves. Water and alcohols are mostly transparent and do not absorb in the UV-vis range and so are excellent mediums for UV-visible spectroscopy. Acetone and dimethylformamide (DMF) are good solvents for compounds insoluble in water and alcohol, but they absorb light below 320 and 275 nm, respectively, so are appropriate only above these cut-off wavelengths.
Enzymes principles and applications Likhith KLIKHITHK1
Enzymes are biological catalysts (also known as biocatalysts) that speed up biochemical reactions in living organisms. They can also be extracted from cells and then used to catalyse a wide range of commercially important processes. For example, they have important roles in the production of sweetening agents and the modification of antibiotics, they are used in washing powders and various cleaning products, and they play a key role in analytical devices and assays that have clinical, forensic and environmental applications. The word ‘enzyme’ was first used by the German physiologist Wilhelm Kühne in 1878, when he was describing the ability of yeast to produce alcohol from sugars, and it is derived from the Greek words en (meaning ‘within’) and zume (meaning ‘yeast’).In the late nineteenth century and early twentieth century, significant advances were made in the extraction, characterization and commercial exploitation of many enzymes, but it was not until the 1920s that enzymes were crystallized, revealing that catalytic activity is associated with protein molecules. For the next 60 years or so it was believed that all enzymes were proteins, but in the 1980s it was found that some ribonucleic acid (RNA) molecules are also able to exert catalytic effects.These RNAs, which are called ribozymes, play an important role in gene expression. In the same decade, biochemists also developed the technology to generate antibodies that possess catalytic properties. These so-called ‘abzymes’ have significant potential both as novel industrial catalysts and in therapeutics. Notwithstanding these notable exceptions, much of classical enzymology, and the remainder of this essay, is focused on the proteins that possess catalytic activity.As catalysts, enzymes are only required in very low concentrations, and they speed up reactions without themselves being consumed during the reaction.
Cheese is a very popular food produced worldwide from the milk of ruminants using a combination of physical treatments. Key milk components for the transformation of milk into curd are casein and calcium. The majority of cheese varieties are based on the curd of modified casein micelles that result from the enzymatic rennet clotting of milk in the presence of calcium ions. The remarkable ability of the spontaneous syneresis of rennet-induced curds can be adjusted to the desired level by biological acidification, cutting, stirring, heating, pressing and salting in order to achieve the desired level of water removal in the form of whey. The mode of curdling (acid or rennet coagulation), the conditions, and the combinations of curd treatments result in numerous cheese varieties with different appearances, textures, flavors and shelf lives. Moreover, most of them are kept under specific temperature and humidity conditions to ripen for a short or a considerable amount of time. The classification of cheese varieties is not unambiguous and can be based on various criteria. For example, cheeses can be classified according to their moisture content related to yield and shelf life or according to specific features related to the treatments applied during cheesemaking and ripening. During ripening, the main solid constituents of young cheese—fat and caseins—undergo changes that increase the concentration of small size compounds in cheese—such as peptides, amino acids, small volatile molecules—control moisture loss and configure textural properties. In particular, the compounds of mature cheese flavor result from complicated biochemical pathways that take place during cheese ripening or even storage.
The function of the fermenter or bioreactor is to provide a suitable environment in which an organism can efficiently produce a target product—the target product might be cell biomass,metabolite and bioconversion Product. It must be so designed that it is able to provide the optimum environments or conditions that will allow supporting the growth of the microorganisms. The design and mode of operation of a fermenter mainly depends on the production organism, the optimal operating condition required for target product formation, product value and scale of production.
The choice of microorganisms is diverse to be used in the fermentation studies. Bacteria, Unicellular fungi, Virus, Algal cells have all been cultivated in fermenters. Now more and more attempts are tried to cultivate single plant and animal cells in fermenters. It is very important for us to know the physical and physiological characteristics of the type of cells which we use in the fermentation. Before designing the vessel, the fermentation vessel must fulfill certain requirements that is needed that will ensure the fermentation process will occur efficiently. Some of the actuated parameters are: the agitation speed, the aeration rate, the heating intensity or cooling rate, and the nutrients feeding rate, acid or base valve. Precise environmental control is of considerable interest in fermentations since oscillations may lower the system efficiency, increase the plasmid instability and produce undesirable end products.
Penicillin is one of the most commonly used antibiotics globally, as it has a wide range of clinical indications. Penicillin is effective against many different types of infections involving gram-positive cocci, gram-positive rods (e.g., Listeria), most anaerobes, and gram-negative cocci (e.g., Neisseria). Importantly, certain bacterial species have obtained penicillin resistance, including enterococci. Enterococci infections now receive treatment with a combination of penicillin and streptomycin or gentamicin. Certain gram-negative rods are also resistant to penicillin due to penicillin’s poor ability to penetrate the porin channel. However, later generations of broad-spectrum penicillins are effective against gram-negative rods. Second-generation penicillins (ampicillin and amoxicillin) can also penetrate the porin channel, making these drugs effective against Proteus mirabilis, Shigella, H. influenzae, Salmonella, and E. coli. Third-generation penicillins such as carbenicillin and ticarcillin are also able to penetrate gram-negative bacterial porin channels. Fourth-generation penicillins such as piperacillin are effective against the same bacterial strains as third-generation penicillins as well as Klebsiella, enterococci, Pseudomonas aeruginosa, and Bacteroides fragilis.
Beer is one of the oldest and most widely consumed alcoholic drinks in the world, and the third most popular drink overall after water and tea. Beer is brewed from cereal grains most commonly from malted barley, though wheat, maize (corn), and rice are also used. The process of beer production is known as brewing. Word brewing is derived from “Bieber” its means to drink.
Brewing is a complex fermentation process. It differs from other industrial fermentation because flavor, aroma, clarity, color, foam production, foam stability and percentage of alcohol are the factors associated with finished product.
During the brewing process, fermentation of the starch sugars in the wort produces ethanol and carbonation in the resulting beer. Most modern beer is brewed with hops, which add bitterness and other flavors and act as a natural preservative and stabilizing agent. Other flavoring agents such as gruit, herbs, or fruits may be included or used instead of hops.
Chromatography is based on the principle where molecules in mixture applied onto the surface or into the solid, and fluid stationary phase (stable phase) is separating from each other while moving with the aid of a mobile phase.
The factors effective on this separation process include molecular characteristics related to adsorption (liquid-solid), partition (liquid-solid), and affinity or differences among their molecular weights
Because of these differences, some components of the mixture stay longer in the stationary phase, and they move slowly in the chromatography system, while others pass rapidly into mobile phase, and leave the system faster.
The word "vitamin" comes from the Latin word “vita”, means "life". Vitamins are organic components in food that are required in very small amounts for growth and for maintaining good health. Vitamins are chemicals found in very small amounts in many different foods Vitamins and minerals are measured in a variety of ways. The most common are:
mg – milligram (a milligram is one thousandth of a gram)
mcg – microgram (a microgram is one millionth of a gram. 1,000 micrograms is equal to one milligram)
IU – international unit (the conversion of milligrams and micrograms into IU depends on the type of vitamin or drug)
(May 29th, 2024) Advancements in Intravital Microscopy- Insights for Preclini...Scintica Instrumentation
Intravital microscopy (IVM) is a powerful tool utilized to study cellular behavior over time and space in vivo. Much of our understanding of cell biology has been accomplished using various in vitro and ex vivo methods; however, these studies do not necessarily reflect the natural dynamics of biological processes. Unlike traditional cell culture or fixed tissue imaging, IVM allows for the ultra-fast high-resolution imaging of cellular processes over time and space and were studied in its natural environment. Real-time visualization of biological processes in the context of an intact organism helps maintain physiological relevance and provide insights into the progression of disease, response to treatments or developmental processes.
In this webinar we give an overview of advanced applications of the IVM system in preclinical research. IVIM technology is a provider of all-in-one intravital microscopy systems and solutions optimized for in vivo imaging of live animal models at sub-micron resolution. The system’s unique features and user-friendly software enables researchers to probe fast dynamic biological processes such as immune cell tracking, cell-cell interaction as well as vascularization and tumor metastasis with exceptional detail. This webinar will also give an overview of IVM being utilized in drug development, offering a view into the intricate interaction between drugs/nanoparticles and tissues in vivo and allows for the evaluation of therapeutic intervention in a variety of tissues and organs. This interdisciplinary collaboration continues to drive the advancements of novel therapeutic strategies.
Cancer cell metabolism: special Reference to Lactate PathwayAADYARAJPANDEY1
Normal Cell Metabolism:
Cellular respiration describes the series of steps that cells use to break down sugar and other chemicals to get the energy we need to function.
Energy is stored in the bonds of glucose and when glucose is broken down, much of that energy is released.
Cell utilize energy in the form of ATP.
The first step of respiration is called glycolysis. In a series of steps, glycolysis breaks glucose into two smaller molecules - a chemical called pyruvate. A small amount of ATP is formed during this process.
Most healthy cells continue the breakdown in a second process, called the Kreb's cycle. The Kreb's cycle allows cells to “burn” the pyruvates made in glycolysis to get more ATP.
The last step in the breakdown of glucose is called oxidative phosphorylation (Ox-Phos).
It takes place in specialized cell structures called mitochondria. This process produces a large amount of ATP. Importantly, cells need oxygen to complete oxidative phosphorylation.
If a cell completes only glycolysis, only 2 molecules of ATP are made per glucose. However, if the cell completes the entire respiration process (glycolysis - Kreb's - oxidative phosphorylation), about 36 molecules of ATP are created, giving it much more energy to use.
IN CANCER CELL:
Unlike healthy cells that "burn" the entire molecule of sugar to capture a large amount of energy as ATP, cancer cells are wasteful.
Cancer cells only partially break down sugar molecules. They overuse the first step of respiration, glycolysis. They frequently do not complete the second step, oxidative phosphorylation.
This results in only 2 molecules of ATP per each glucose molecule instead of the 36 or so ATPs healthy cells gain. As a result, cancer cells need to use a lot more sugar molecules to get enough energy to survive.
Unlike healthy cells that "burn" the entire molecule of sugar to capture a large amount of energy as ATP, cancer cells are wasteful.
Cancer cells only partially break down sugar molecules. They overuse the first step of respiration, glycolysis. They frequently do not complete the second step, oxidative phosphorylation.
This results in only 2 molecules of ATP per each glucose molecule instead of the 36 or so ATPs healthy cells gain. As a result, cancer cells need to use a lot more sugar molecules to get enough energy to survive.
introduction to WARBERG PHENOMENA:
WARBURG EFFECT Usually, cancer cells are highly glycolytic (glucose addiction) and take up more glucose than do normal cells from outside.
Otto Heinrich Warburg (; 8 October 1883 – 1 August 1970) In 1931 was awarded the Nobel Prize in Physiology for his "discovery of the nature and mode of action of the respiratory enzyme.
WARNBURG EFFECT : cancer cells under aerobic (well-oxygenated) conditions to metabolize glucose to lactate (aerobic glycolysis) is known as the Warburg effect. Warburg made the observation that tumor slices consume glucose and secrete lactate at a higher rate than normal tissues.
This pdf is about the Schizophrenia.
For more details visit on YouTube; @SELF-EXPLANATORY;
https://www.youtube.com/channel/UCAiarMZDNhe1A3Rnpr_WkzA/videos
Thanks...!
Multi-source connectivity as the driver of solar wind variability in the heli...Sérgio Sacani
The ambient solar wind that flls the heliosphere originates from multiple
sources in the solar corona and is highly structured. It is often described
as high-speed, relatively homogeneous, plasma streams from coronal
holes and slow-speed, highly variable, streams whose source regions are
under debate. A key goal of ESA/NASA’s Solar Orbiter mission is to identify
solar wind sources and understand what drives the complexity seen in the
heliosphere. By combining magnetic feld modelling and spectroscopic
techniques with high-resolution observations and measurements, we show
that the solar wind variability detected in situ by Solar Orbiter in March
2022 is driven by spatio-temporal changes in the magnetic connectivity to
multiple sources in the solar atmosphere. The magnetic feld footpoints
connected to the spacecraft moved from the boundaries of a coronal hole
to one active region (12961) and then across to another region (12957). This
is refected in the in situ measurements, which show the transition from fast
to highly Alfvénic then to slow solar wind that is disrupted by the arrival of
a coronal mass ejection. Our results describe solar wind variability at 0.5 au
but are applicable to near-Earth observatories.
Observation of Io’s Resurfacing via Plume Deposition Using Ground-based Adapt...Sérgio Sacani
Since volcanic activity was first discovered on Io from Voyager images in 1979, changes
on Io’s surface have been monitored from both spacecraft and ground-based telescopes.
Here, we present the highest spatial resolution images of Io ever obtained from a groundbased telescope. These images, acquired by the SHARK-VIS instrument on the Large
Binocular Telescope, show evidence of a major resurfacing event on Io’s trailing hemisphere. When compared to the most recent spacecraft images, the SHARK-VIS images
show that a plume deposit from a powerful eruption at Pillan Patera has covered part
of the long-lived Pele plume deposit. Although this type of resurfacing event may be common on Io, few have been detected due to the rarity of spacecraft visits and the previously low spatial resolution available from Earth-based telescopes. The SHARK-VIS instrument ushers in a new era of high resolution imaging of Io’s surface using adaptive
optics at visible wavelengths.
Introduction:
RNA interference (RNAi) or Post-Transcriptional Gene Silencing (PTGS) is an important biological process for modulating eukaryotic gene expression.
It is highly conserved process of posttranscriptional gene silencing by which double stranded RNA (dsRNA) causes sequence-specific degradation of mRNA sequences.
dsRNA-induced gene silencing (RNAi) is reported in a wide range of eukaryotes ranging from worms, insects, mammals and plants.
This process mediates resistance to both endogenous parasitic and exogenous pathogenic nucleic acids, and regulates the expression of protein-coding genes.
What are small ncRNAs?
micro RNA (miRNA)
short interfering RNA (siRNA)
Properties of small non-coding RNA:
Involved in silencing mRNA transcripts.
Called “small” because they are usually only about 21-24 nucleotides long.
Synthesized by first cutting up longer precursor sequences (like the 61nt one that Lee discovered).
Silence an mRNA by base pairing with some sequence on the mRNA.
Discovery of siRNA?
The first small RNA:
In 1993 Rosalind Lee (Victor Ambros lab) was studying a non- coding gene in C. elegans, lin-4, that was involved in silencing of another gene, lin-14, at the appropriate time in the
development of the worm C. elegans.
Two small transcripts of lin-4 (22nt and 61nt) were found to be complementary to a sequence in the 3' UTR of lin-14.
Because lin-4 encoded no protein, she deduced that it must be these transcripts that are causing the silencing by RNA-RNA interactions.
Types of RNAi ( non coding RNA)
MiRNA
Length (23-25 nt)
Trans acting
Binds with target MRNA in mismatch
Translation inhibition
Si RNA
Length 21 nt.
Cis acting
Bind with target Mrna in perfect complementary sequence
Piwi-RNA
Length ; 25 to 36 nt.
Expressed in Germ Cells
Regulates trnasposomes activity
MECHANISM OF RNAI:
First the double-stranded RNA teams up with a protein complex named Dicer, which cuts the long RNA into short pieces.
Then another protein complex called RISC (RNA-induced silencing complex) discards one of the two RNA strands.
The RISC-docked, single-stranded RNA then pairs with the homologous mRNA and destroys it.
THE RISC COMPLEX:
RISC is large(>500kD) RNA multi- protein Binding complex which triggers MRNA degradation in response to MRNA
Unwinding of double stranded Si RNA by ATP independent Helicase
Active component of RISC is Ago proteins( ENDONUCLEASE) which cleave target MRNA.
DICER: endonuclease (RNase Family III)
Argonaute: Central Component of the RNA-Induced Silencing Complex (RISC)
One strand of the dsRNA produced by Dicer is retained in the RISC complex in association with Argonaute
ARGONAUTE PROTEIN :
1.PAZ(PIWI/Argonaute/ Zwille)- Recognition of target MRNA
2.PIWI (p-element induced wimpy Testis)- breaks Phosphodiester bond of mRNA.)RNAse H activity.
MiRNA:
The Double-stranded RNAs are naturally produced in eukaryotic cells during development, and they have a key role in regulating gene expression .
Nutraceutical market, scope and growth: Herbal drug technologyLokesh Patil
As consumer awareness of health and wellness rises, the nutraceutical market—which includes goods like functional meals, drinks, and dietary supplements that provide health advantages beyond basic nutrition—is growing significantly. As healthcare expenses rise, the population ages, and people want natural and preventative health solutions more and more, this industry is increasing quickly. Further driving market expansion are product formulation innovations and the use of cutting-edge technology for customized nutrition. With its worldwide reach, the nutraceutical industry is expected to keep growing and provide significant chances for research and investment in a number of categories, including vitamins, minerals, probiotics, and herbal supplements.
Body fluids_tonicity_dehydration_hypovolemia_hypervolemia.pptx
Fluorescence microscopy Likhith K
1. FLUORESCENCE MICROSCOPY
By
Mr. LIKHITH K
(Research Scholar)
Department of Biomedical Engineering
Manipal Institute of Technology
Eshwar Nagar, Manipal, Karnataka-
576104
3. INTRODUCTION
Fluorescence microscopy provides an efficient and unique approach to study fixed and living cells because of its
versatility, specificity, and high sensitivity.
Fluorescence microscopes can both detect the fluorescence emitted from labeled molecules in biological samples
as images or photometric data from which intensities and emission spectra can be deduced.
By exploiting the characteristics of fluorescence, various techniques have been developed that enable the
visualization and analysis of complex dynamic events in cells, organelles, and sub-organelle components within
the biological specimen.
The most common techniques are
1) Fluorescence recovery after photo bleaching (FRAP)
2) Fluorescence loss in photo bleaching (FLIP)
3) Fluorescence localization after photo bleaching (FLAP)
4) Fluorescence resonance energy transfer (FRET)
And the different ways to measure FRET are such as
1) Acceptor bleaching
2) Sensitized emission
3) Polarization anisotropy
4) Fluorescence lifetime imaging microscopy (FLIM)
4. The Physical Phenomenon of Fluorescence
Fluorescence as a phenomenon is part of a larger family of related luminescent processes in which a susceptible
substance absorbs light, only to reemit light (photons) from electronically excited states after a given time (Figure
1).
Photo luminescent processes that are generated through excitation, whether this is via physical, mechanical, or
chemical mechanisms, can generally be subdivided into fluorescence and phosphorescence.
Absorption of a light quantum (blue) causes an electron to move to a higher energy orbit. After residing in this
“excited state” for a particular time, the fluorescence lifetime, the electron falls back to its original orbit and the
fluorochrome dissipates the excess energy by emitting a photon (green).
Figure1 Schematic representation of the fluorescence phenomenon in the classical Bohr model.
5. Compounds that display fluorescent properties are generally termed fluorescent probes or dyes.
Often ‘fluorochrome’ and ‘fluorophore’ are used interchangeably.
The term ‘fluorophore’ refers to fluorochromes that are conjugated covalently or through adsorption to biological
macromolecules, such as nucleic acids, lipids, or proteins.
Fluorochromes come in different flavors and include
1) organic molecules (dyes)
2) inorganic ions (e.g., lanthanide ions such as Eu, Tb, Yb, etc.)
3) fluorescent proteins (e.g., green fluorescent protein)
4) atoms (such as gaseous mercury in glass light tubes)
Some commonly used fluorochromes are listed in Table 1 and 2.
Recently, inorganic luminescent semiconducting nanoparticles, quantum dots, have been introduced as labels for
biological assays, bio-imaging applications, and theragnostic purposes (the combination of diagnostic and
therapeutic modalities in one and the same particle).
6. Table 1 Some fluorochromes used to label proteins
7. Table 2 Some fluorochromes used to stain nucleic acids fluorochrome abbreviation absorption emission
8. Fluorescence follows a series of discrete steps of which the outcome is the emittance of a photon with a longer
wavelength
Figure 2 Process which can be visualized in more detail via the Jabłoński diagram
9. When light of a particular wavelength hits a fluorescent sample, the atoms, ions or molecules therein absorb a
specific quantum of light, which pushes a valence electron (outer most shell electrons) from the ground
state (GS0).
This initial state is an electronic singlet in which all electrons have opposite spin and the net spin is 0
Jumping into a higher energy level , creating an excited state (Esn).
This process is fast and in the femtosecond range and requires at least the energy to bridge the gap between
excited and ground states in order for excitation to occur.
ΔE = EESn − EGS0
The energy of photons involved in fluorescence and generally a quantum of light can be expressed via Planck’s
law :
E =hv = h (c/λ)
where E is the quantum’s energy (J)
h is Planck's constant (J.s)
ν the frequency (s−1)
λ is the wavelength of the photon (m)
c is the speed of light (m.s−1)
However, there are several excited state sublevels (vibrational levels) and which level is reached primarily
depends on the fluorescent species’ properties.
10. After excitation to the higher energy level ESn, the electron quickly relaxes to the lowest possible excited
sublevel, which is in the picosecond range.
The energy decay from dropping to a lower vibrational sublevel occurs through intramolecular non-radiative
conversions and the converted heat is absorbed via collision of the excited state fluorescent molecule with the
solvent molecules.
Emission spectra are usually independent of the excitation wavelength because of this rapid relaxation to the
lowest vibrational level of the excited state, which is known, as Kasha’s rule. In most cases, absorption and
emission transitions involve the same energetic levels as schematically shown in Figure 3.
For this reason and the fact that excitation is instantaneous, involving electrons only and leaving the heavier
nuclei in place, many fluorochromes display near mirror image absorption and emission spectra (mirror image
rule), although many exceptions exist.
Intersystem crossing is the slowest energy dissipation pathway, because the electron has to change spin
multiplicity from an excited singlet state to an excited triplet state (Figure 2 B).
Intersystem crossing is mostly observed in molecules containing heavy atoms such as iodine or bromine or in
paramagnetic species.
11. Figure 3 Absorption and emission transitions involve the same energetic levels as schematically shown below.
12. The difference between the excitation and emission maxima is called “Stokes shift”.
It is caused by a quick electron relaxation and intramolecular vibrational energy loss taking place between the
different excited state sublevels.
That is the reason why the excitation light normally has a shorter wavelength (i.e., higher energy) than the
emission light (i.e., lower energy).
In many fluorochromes, the same electronic transitions are involved in both excitation and emission, which leads
to near-mirror image spectra.
Lanthanide ions are good examples of luminescent probes that show delayed fluorescence.
The term “luminescence” is normally used when discussing lanthanide-based emission, because “fluorescence”
refers to spin allowed singlet-to-singlet emission, whereas in lanthanide ions, emission is due to intra-
configurational f-f transitions (transitions inside the 4f shell).
As a result they have fluorescence lifetimes in the (sub)microsecond range for Yb(III) and Nd(III), whereas
Eu(III), Tb(III) and Sm(III) have even longer lifetimes in the (sub)millisecond range.
This is significantly longer than the lifetimes of organic fluorochromes and fluorescent proteins which are
generally in the nanosecond range.
Because of the large lifetime difference to fluorescence, lanthanide emission should easily be distinguishable
from fluorescence emission by time-gating techniques.
13. When the electron finally returns to the lower energy level it originated from, the ground state GS0, a quantum
of light (photon) is emitted with a longer wavelength, which is an allowed transition since the spin is retained.
In most fluorochromes, photon emission is produced by a π*→π or π*→n transition, depending on which
requires the least energy for the transition to occur.
In contrast, σ*→ σ transitions are rare since the required UV light (below 250 nm) is energetic enough to
deactivate the excited state electron by pre dissociation (internal conversion to a GS0 that is at such a high
vibrational level that the bond breaks) or dissociation (the bond breaks at a vibrational excited state).
Photon emittance from singlet states with an average time-scale between 10−9 and 10−6 seconds is slow
compared with the absorption of photons.
This resulting emitted radiation is called fluorescence and in the simplest form of fluorescence microscopy, this
emitted light is collected and transported to the detector through the same objective lens used to focus the
excitation light onto the sample.(Figure 4).
Fluorochromes can enter repetitive cycles of excitation and emission as long as no destruction or covalent
modification occurs that irreversibly interrupts this process.
The transition from the meta-stable triplet state ET1 to the ground state GS0 is, because of the necessary spin
reversal, forbidden and therefore several orders of magnitude slower than fluorescence, i.e., thus called
phosphorescence.
Consequently, the emission takes place over long periods of time in some materials it takes several seconds to
even minutes.
14. Figure 4 In fluorescence microscopy the sample is illuminated with excitation light and the emitted light (the
fluorescence) is detected through the same objective (epi-fluorescence microscopy).
15. Fluorescence emission generally occurs at longer wavelengths and concomitant lower energy than the
light used to excite the fluorochrome, provided that a single photon is involved during excitation.
It was the British scientist Sir George Stokes who first observed fluorescence when irradiating
fluorspar (fluorite) with UV radiation and a red-shift in the resulting emitted light, which he reported
in his 1852 publication “on the change of refrangibility of light”.
The difference between the emission and excitation maxima is called “Stokes shift” (Figure 3).
The Stokes shift varies markedly among different fluorochromes.
Note anti-Stokes shifts in which the emission wavelength is smaller than the excitation wavelength are
also possible, for instance during photon up conversion or two-photon excitation.
Anti-Stokes fluorescence also occurs commonly in fluorochromes in which absorption and emission
spectra overlap substantially.
Therefore fluorochromes not only have characteristic excitation spectra, but also characteristic
emission spectra that are dependent on their specific vibronic configuration and properties.
16. FLUORESCENCE CHARACTERISTICS
Some of the essential characteristics and parameters of fluorescence that are utilized in fluorescence microscopy,
such as
1) The fluorescence life time
2) Quantum yield
3) Anisotropy
4) Quenching
5) Photobleaching
6) Fluorescence intermittency / blinking
7) Autoflurosence
8) Resonance energy transfer
9) Energy transfer
17. 1. Quantum yield:
The quantum yield (Ф) basically determines how bright a fluorochrome’s emission is.
It is given by the ratio of the number of emitted to absorbed photons, which is determined by the rate constants
of emission (Γ) and the sum of all non-radiative decay processes (knr) that depopulate the excited state.
The quantum yield, as many intrinsic fluorescence parameters, is sensitive to environmental influences, such a
solvent polarization, pH, fluorochrome concentration, and the presence of molecules affecting the excited state,
such as molecular oxygen.
18. 2. Fluorescence lifetime:
The fluorochrome’s fluorescence lifetime (τ) is the average time the electron spends in the excited state before
returning to the ground state.
In other words, the depopulation of excited state molecules through radiative (Γ) and non-radiative processes (knr)
follows an exponential decay and the time of this process is basically the fluorescence lifetime
19. 3. Anisotropy:
This refers to the quality of having different properties along different axes: in a pool of randomly oriented
fluorochromes, only those fluorochromes with transition dipole moments that are aligned (near) parallel to the
polarization direction of the excitation beam (linearly polarized) will be excited (photo selection).
Fluorescence polarization is determined by the orientation of the fluorochromes’ transition moment at the instant
of emission, which allows the determination of the fluorochromes’ rotation by measuring their anisotropy.
Theoretically, the maximal anisotropy is achieved when the emission transition dipole moment is exactly
parallel to the absorption transition dipole moment.
20. 4. Fluorescence quenching:
Quenching is a phenomenon by which interaction of a molecule, the quencher, with the fluorochrome reduces
the quantum yield or the lifetime.
Quenching phenomena can be subdivided into:
1) Dynamic quenching occurs through collision of the quencher and the excited state fluorochrome, which leads
to a decrease in the lifetime and emission intensity.
2) Static quenching arises from direct interaction of the fluorochrome and quenching molecules, for instance by
forming a non-fluorescent ground state complex. This form of quenching does not necessarily decrease the
measured emission lifetime and often occurs simultaneous with dynamic quenching.
3) Self-quenching or concentration quenching, the fluorochrome quenches its own fluorescence because of close
proximity of identical molecules at high concentration. Self-quenching occurs in particular in biomembranes,
where the lipid bilayer behaves as a 2D fluid with different domains of fluidity where fluorochromes can be
concentrated or when labeling proteins with multiple labels.
4) Color-quenching is a process in which emitted photons are absorbed by a strongly colored component such as
β-carotene. This leads to a decrease in intensity, but not the fluorescence lifetime.
21. 5. Fluorescence intermittency or “blinking”:
This phenomenon occurs when the fluorochrome randomly alternates between a fluorescent (“on”) and dark
state (“off”) despite continuous excitation illumination.
As a result, when tracking single fluorochromes, a stroboscopic effect may interfere with the tracking procedure.
Blinking generally follows power law statistics and occurs commonly in luminescent nanoparticles, but also in
some organic dyes, and fluorescent proteins.
The random nature and power law dynamics generally frustrates and precludes comparison of results between
independent experiments, because the “on” and “off” time distributions can significantly differ.
22. 6. Autofluorescence:
Fluorescence that does not originate from the fluorochrome of interest (FOI), but rather from cellular
components that have fluorescent properties, most notably flavins, e.g., FAD+ and riboflavin, NAD(P)H, and
extracellular matrix components, e.g., elastin and collagen, but also retinol, folic acid, lipofuscin, and
chlorophyll.
The autofluorescence window approximately encompasses the range from 350 nm to 600 nm and can effectively
be avoided by a number of strategies:
1) Precise filtering of the FOI signal with narrow band pass optical filters,
2) The use of probes that fluoresce outside the autofluorescence window, commonly in the (near) infrared (NIR)
region,
3) The use of time-resolved techniques (autofluorescent bio fluorochromes have distinctly different lifetimes),
4) The use of up converting fluorochromes that allow excitation in the IR; (v) multispectral imaging (recording
spectra in every pixel), and (vi) spectral un mixing (mathematical disentangling of mixed emission signals).
23. 7. Photobleaching:
Photobleaching or “fading” is a photochemical process in which the fluorochrome’s ability to enter repetitive
excitation is permanently interrupted by destruction or irreversible covalent modification of the fluorochrome by
reaction with surrounding biomolecules.
Photodestructive and photochemical processes occur predominantly when the fluorochrome is in the dark triplet
excited state, which is longer lived than singlet states and exhibits a high degree of chemical reactivity.
24. 8. Resonance energy transfer:
This is a photophysical process in which the excited state energy from a donor fluorochrome is transferred via a
non-radiative mechanism to a ground state acceptor chromophore via weak long-range dipole–dipole coupling.
The theoretical basis for the molecular interactions involved in resonance energy transfer was first described by
Theodor Förster in the 1940s.
25. 9. Charge-transfer complexes:
These are nanosecond short-lived homodimers (excimer) or heterodimers (exciplex) of two molecules of which
at least one is in the excited state that show red-shifted emission compared with the monomer’s emission.
Such complexes occur via electrostatic attraction because of partial electronic charge transfer between the
individual entities.
The individual ground state monomers would normally not associate and the monomers in the complex
dissociate and repel each other once relaxation to the ground state occurs.
Since these complexes require close proximity, excimer and exciplex formation require high concentrations of
the monomers.
26. BRIEF HISTORY
The first fluorescence microscopes were developed at the beginning of the 20th century.
In 1904, August Köhler constructed an ultraviolet (UV) illumination microscope at Zeiss Optical Works in Jena,
Germany, in which he used a cadmium arc lamp as a light source.
However, it was Oskar Heimstädt who developed the first working fluorescence microscope in 1911, with which
he studied autofluorescence in organic and inorganic compounds .
Still, these early fluorescence microscopes suffered from several drawbacks, including the fact that the light
sources at that time did not have enough power to excite fluorochromes at high enough rates and that effective
separation of the fluorescence signal from the excitation light was difficult to achieve.
In order to obtain sufficient signal, Heimstädt had to rely on darkfield illumination, which ensured that only a
limited amount of excitation light would enter the objective lens, but this was a technically challenging method
and certainly not suited for developing fluorescence microscopy as a mainstream tool.
The invention of the epi-fluorescence microscope in 1929 by Philipp Ellinger and August Hirt was a major step
forward to achieving this goal.
27. Figure 5 Anatomy of an epi-illumination fluorescence microscope.
28. In the 1930s the Austrian Max Haitingen and others developed the technique of ‘secondary fluorescence’ in
which samples were systematically stained with fluorescent dyes, initially simply to make the weak
autofluorescent biological samples better visible.
Haitingen also was the first to introduce the word ‘fluorochrome’ for these fluorescent stains.
In the early 1940s, Albert Coons developed the technique of labeling antibodies with fluorescent dyes . This was
a breakthrough, as it allowed to specifically label proteins and subcellular structures and as a result made these
molecular structures visible in a contrast and resolution never seen before.
Since these first experiments, antibody staining with fluorescent secondary markers has become a standard
method in biological and biomedical research, and clinical diagnostics for fixed samples, including tissues and
single cells.
Furthermore, a significant increase in fluorescence signal can be achieved with these fluorochromes over the
weak autofluorescent endogenous biological species.
The lack of excitation power was resolved with the development of lasers in the 1960s based on Einstein’s
theoretical foundations regarding stimulated emission by Gould, Townes, Schawlow, and Maiman.
Lasers offered what other light sources could not: a high degree of spatial and temporal coherence, which means
that the diffraction limited monochromatic and coherent beam can be focused in a tiny spot, achieving a very high
local irradiance.
Furthermore, it now became possible to effectively separate signals by using suitable filters and dichroic mirrors
(also called dichromatic beam splitters). (figure 5)
The latter are specialized interference filters that selectively allow passage of light in a particular wavelength
range, while reflecting other wavelengths when placed into the light path at a 45° angle (Figure 5).
29. GREEN FLUORESCENT PROTEIN (GFP)
The next foremost breakthrough that resulted in an explosion in both instrument and technique development and
concurrently biological research was the discovery in the 1960s, sequencing and subsequent development of
green fluorescent protein (GFP) as a fluorescent label in the 1990s by Tsien, Chalfie, and Shimomura.
GFP is a 238 amino acid protein that shows bright green fluorescence and was first isolated from the
jellyfish Aequorea victoria.
The 26.9 kDa wild-type GFP consists of a β-barrel structure (Figure 6) in which the essential chromophoric
moiety, an amino acid triplet of Ser65, Tyr66, and Gly67, lies at the centre.
The entire poly-peptide structure is necessary for GFP fluorescence, the chromophore forms autocatalytically and
that the molecular structure surrounding the tripeptide influences its fluorescent properties.
Furthermore, the protective β-barrel surrounding the tripeptide ensures stability, makes GFP relatively insensitive
to environmental influences, and causes physical separation from species such as molecular oxygen.
As a result, GFP’s photobleaching rate is lower than those of conventional fluorochromes.
Wild-type GFP (from A. victoria) fluorescence is characterized by a major excitation peak at 395 nm and a minor
one at 475 nm (Figure 6), which results in bright green emission at 509 nm and a quantum yield of 0.77.
30. Figure 6 Molecular structure and localization of the chromophoric
tripeptide in A. victoria wild-type GFP.
31. Many fluorescent proteins (FPs) from other species, such as the Anthozoan button polyp Zoanthus (ZsYellow),
sea anemone Discosoma (DsRed), or Anemonia majano (AmCyan1), have been identified and isolated, which
now results in a wide color palette, with various photostabilities, sensing properties, photo-switchability, and
useful FRET pairs.
32. The development of FP technology was so significant that it opened the doors to completely new ways of
performing fluorescence live cell imaging, particularly since it was now possible to tailor the fluorescent label’s
properties through genetic engineering and to label proteins by expressing fluorescent fusion constructs directly
in living cells.
Bio nanotechnology over the past decades resulted in the development of luminescent nanoparticles with
exceptional physical and chemical properties, not seen in other fluorochromes.
Quantum dots (QDs), for instance, are inorganic semiconducting nanoparticles consisting of a core-shell
configuration creating a spectral bandgap, e.g., CdSe/ZnS QDs.
QDs have a relatively long lifetime, which provides the possibility to correct for background signals from short
lived fluorescent species by time-gating techniques.
QDs have broad absorption spectra, a single light source can be used to excite multiple QDs with different
emission wavelengths simultaneously.
Quantum dots are characterized by a number of additional unique properties
1) QDs are about 10–100 times brighter than organic fluorogenic dyes
2) They are 100–1,000 times more resistant to photobleaching, because the shell and various coatings form
physical barriers that separate the excited state from surrounding biomolecules and molecular oxygen
3) They show narrower and more symmetric emission spectra compared with other fluorochromes.
33. Fluorescence microscopy is the method of choice for live cell imaging and it is a standard procedure to study
normal and pathological cell biological processes in single cells, subcellular compartments or across a population
of cells by introducing fluorochromes specifically targeted to the (bio)molecules of interest.
Major advantages are that fluorescence microscopy techniques provide information with spatio-temporal
resolution and are generally less destructive compared with other imaging techniques, e.g., Electron Microscopy
(EM).
34. What makes fluorescence microscopy such a great and specific tool for cellular and molecular imaging and analysis?
Essentially it is its selectivity and contrast enhancement.
While the selectivity is achieved predominantly through the labeling methods
The contrast increase is realized in the microscope itself.
Modern fluorescence microscopes can maximize the collection of emitted fluorescent light, while minimizing the collection
of the incident excitation light.
The main advantages of fluorescence microscopy is the dramatic increase in signal from the labeled structures and molecules
against a dark background
Image contrast critically dependents on the ability of the microscope to pass fluorescent light to the detector while blocking
the excitation light.
Due to its selectivity and contrast, not only fine cellular and subcellular structures, but even single molecules can be made
visible in the fluorescence microscope.
If they are spatially well separated and thus not too close to each other or do not light up at the same time, localization of
individual molecules is feasible, but is diffraction limited.
Three basic components are present in every light microscope, irrespective of the type:
1) An illumination source
2) A magnifying lens
3) An image acquisition device.
35. In a wide field fluorescence microscope, the white light source is replaced by a high power lamp (a mercury or
xenon source), which excites the fluorochromes in the fluorescently labeled sample and induces fluorescence
emittance(Figure 5).
Images are typically acquired visually by eye or electronically with a CCD camera.
Fluorochromes have characteristic excitation spectra.
Thus, an appropriate excitation filter, usually a band-pass filter (BP), is placed between the lamp and the sample
to narrow the wavelength range of light reaching the sample to such an extent that the fluorochromes used are
excited efficiently, whereas unwanted excitation is minimized. (Figure 7)
Since the emitted light has a longer wavelength than the excitation light, an emission filter (either a long pass
[LP] or BP filter) placed between the sample and the detector effectively blocks the excitation light and prevents
perturbation of the final image.
Intense light is required for successful fluorescence excitation.
Lasers generally produce high intensity light and have proven to be an excellent alternative excitation source to
mercury and xenon lamps.
Since lasers are a source of monochromatic light, generally no excitation filter is required.
However an emission filter or an alternative spectral selection device is still needed to stop the excitatory laser
light from reaching the detector and to tune in on the fluorochrome’s emission signal, especially in multiple
labeling experiments.
37. RESOLUTION IN FLUORESCENCE MICROSCOPY
In fluorescence microscopy, the optical resolving power determines the amount of detail observed in a specimen,
which in turn is determined by a number of physical factors and instrument limitations.
In order to obtain sharp images, the objective must capture as much of the deflected light as possible, which is
achieved with wide angular openings (aperture).
Ernst Abbe first defined the numerical aperture (N.A.), which determines the objective’s light capturing capacity
and can mathematically be written as
Where, n is the refraction index of the medium between the object and the objective (n = 1 for air and for
immersion oil n = 1.51)
α is half the objective opening angle.
38. To maximize capturing the deflected light and to increase the resolution, several strategies can be employed,
including the use of a condenser lens for illumination to widen the angle of the ray cone on the illumination side
and or to use an immersion liquid between objective lens and the cover slip, which abrogates reflections that
normally diminish the resolving power.
In fluorescence microscopy the resolution is not directly governed by the magnification. Resolution and contrast
are two reciprocally interrelated parameters that are important in fluorescence microscopy and should not be
considered as separate entities.
Individual objects in a specimen cause diffraction of light and as a result, an illuminated point source within the
specimen is observed as a bright central spot (Airy disc) with surrounding diffraction rings (Airy pattern) as
shown in Figure 7.
Figure 7 Airy disc diffraction pattern
39. Essentially, resolution may be defined as the smallest distance between two points in the specimen that can still
be discriminated as separate points at a particular contrast, which with Equation 5 can be written as:
40. Contrast is defined as the difference between the maximum intensity and minimum intensity occurring
in the space between two objects of equal intensity.
When the two point objects are well separated, the contrast minimum between them is near zero and
the objects can be discriminated .
However, as the point objects approach and their PSFs start to overlap, the intensity minimum between
the two object maxima is reduced until the objects are no longer resolved.
Rayleigh criterion for resolution
Which states that two points are resolved when the first minimum of one Airy disc is aligned with the
central maximum of the second Airy disc.
From the above mentioned statement , it becomes obvious that the smaller the Airy pattern, the higher
the resolution.
41. SAMPLE PREPARATION
Fluorescence from a fluorophore tagged to a molecule of interest is often used to measure the quantity of the
tagged molecule.
Fluorescent proteins expressed in live cells are excellent for quantitation; because there is a constant number of
fluorophores per labeled protein.
The number of photons emitted can be an accurate measure of the quantity of fluorescently labeled protein.
Quantitation of live versus fixed cells is generally preferable because the fixation and extraction process can
remove tagged proteins, quench the fluorescence of fluorescent proteins, and change the size and shape of cells.
The fixation and extraction necessary to get antibodies into cells can change the quantity and localization of
detectable epitopes.
Measuring fluorescence deep into specimens can also be problematic for measurements of signal intensities.
In biological specimens, light scattering and optical aberrations increase with distance from the coverslip and
decrease signal intensity.
These effects are difficult to characterize and correct for in inhomogeneous biological samples.
Although the effects of light scattering are minimized when using multi-photon illumination.
43. CONCLUSION
The significance of imaging-based methodologies is underscored by the fact that the major part of
discoveries in life sciences over at least the past 50 years were based on imaging biological and
pathological processes.
The advanced fluorescence microscopic techniques has a major impact on cell biological research and
(bio)medicine.
Nowadays functional insight in cellular processes that was previously the mainstay of analytical
biochemistry and could only be observed on gels and blots can now directly be visualized and also be
analyzed in the living cell.
Fluorescence microscopy is a valuable toolbox to study cellular structures and dynamics spanning
scales from the single molecule to the live animal.
The spatial resolution that can be achieved with any light-based microscopy is however limited to
about 200 nm in the imaging plane and >500 nm along the optical axis.
It has been a motivation and a challenge to bypass this limit in spatial resolution, and to extend the
range of fluorescence microscopy reaching a near-molecular resolution.
It’s a selection of techniques that successfully demonstrated sub-diffraction resolution fluorescence
imaging and which today are used for imaging of small cellular structures.
However, even though techniques such as FRAP, FLIP, and FRET have become more common place
in life science research, they are certainly not trivial methodologies with many possible pitfalls, some
of which are obvious, whilst others are more obscure.
44. REFERENCE
Hellen C. Ishikawa-Ankerhold etal. 2012,Advanced Fluorescence Microscopy Techniques-FRAP, FLIP, FLAP,
FRET and FLIM. 17(4): 4047–4132.
Berezin M.Y., Achilefu S. Fluorescence lifetime measurements and biological imaging. Chem.
Rev. 2010;110:2641–2684
Lakowicz J.R. Principles of Fluorescence Spectroscopy. 3rd. Springer Science; New York, NY, USA: 2006
Wang Y.L. Fluorescence Microscopy of Living Cells in Culture. Part A. Fluorescent Analogs, Labelling Cells,
and Basic Microscopy. Methods in Cell Biology. Vol. 29 Academic Press; San Diego, State abbr., USA: 1989
Swift S.R., Trinkle-Mulcahy L. Basic principles of FRAP, FLIM and FRET. Proc. Royal Mic. Soc. 2004;39:3–
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