Alanylalanine
It is involved in various biological processes and has potential applications in research and clinical settings.
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Most cited protocols related to «Alanylalanine»
EXAMPLE 1
The peptide to be immobilized H-Ala-Ala-OH was combined as the alanylalanine methyl ester hydrochloride 2 (7.2 g) with 10 g of L-N-Boc-2-(2-oxo-2-phenylethyl) glycine 1, i.e., with a linker compound of the general formula (I) (compare
Ethyl diisopropylamine (1.3 ml) was slowly dripped into this suspension while stirring at 0° C. (ice cooling). The suspension was heated to room temperature and stirring was continued, until compound 1 could still be detected only in trace amounts, by thin-layer chromatography (silica gel 60 F254, mobile phase: dichloromethane/methanol 10:1) (approximately 2 h). The mixture was placed in a separatory funnel and the organic phase was extracted sequentially with 500 ml each of water, saturated tartaric acid solution and saturated sodium hydrogen carbonate solution. The organic phase was separated, dried with sodium sulfate, and the solvent was removed on the rotary evaporator. Approximately 15 g of a resin were obtained, which were purified on silica gel 60 (mobile phase: dichloromethane/methanol 5:1) by flash column chromatography. The yield of 2-[2-(2-tert-butoxycarbonylamino-4-oxo-4-phenyl-butyrylamino)propionylamino] propionic acid methyl ester 3 (Boc-BzAla-Ala-Ala-OMe) amounted to 13 g.
A polypropylene membrane (diameter 30 mm) was immersed for 30 minutes in a 0.1 M solution of 2-[2-(2-tert-butoxycarbonylamino-4-oxo-4-phenylbutyrylamino)propionylamino]propionic acid methyl ester 3, i.e., a photoreactive amino acid of the general formula (II) (compare
The membrane was irradiated for 30 minutes with the light of an HBO 500 at a distance of 20 cm with the use of a cutoff filter, which filters out light below 290 nm.
The membrane was then washed five times with a total of 150 ml of dichloromethane and dried for 30 minutes in high vacuum at 3·10−5 Torr.
The immobilization of the peptide according to formula (IV), in which the radicals R1 und R3 and the biomolecule M have the above-named meanings, was detected by comparison of the FT-IR spectra for the polypropylene membrane before and after treatment.
EXAMPLE 2
A polypropylene membrane (diameter 30 mm) was irradiated in a glass dish, filled with a 0.1 M solution of 2-[2-(2-tert-butoxycarbonylamino-4-oxo-4-phenylbutyrylamino)propionylamino]propionic acid methyl ester 3 (produced according to Example 1), i.e., a photoreactive amino acid of the general formula (II), with R1=phenyl and R3=t-butoxycarbonyl (Boc), and peptide H-Ala-Ala-OH bound to the N terminal as the methyl ester in benzene, for 60 minutes with the light of an HBO 500 at a distance of 20 cm with the use of a tilted mirror and a cutoff filter, which filters out light below 290 nm.
The membrane was then washed once with 50 ml of benzene and twice with 50 ml of dichloromethane and dried for 30 minutes in high vacuum at 3·10−5 Torr.
The immobilization of the peptide according to formula (IV), in which the radicals R1 and R3 have the above-named meanings, was detected by comparison of the FT-IR spectra for the polypropylene membrane before and after treatment.
In the spectrometer, a weak reflection90 (link),91 (link) from a wedged ZnSe window is used as probe beam. The transmitted IR light is guided to a pulse shaper, where it is diffracted from a grating (150 l/mm), collimated using a parabolic mirror, and guided to a Germanium-based acousto-optic modulator (AOM). The IR light is diffracted at the AOM and focused onto a second grating (150 l/mm). The shaped beam is reflected from a retroreflector on a translational stage to control the waiting time (T2) between the pump and the probe beams. After setting the polarization of the pump beam to 45° relative to the probe beam polarization, the pump and the probe beams are focused into the sample using an off-axis parabolic mirror. After the sample, the probe beam is re-collimated and split into polarization components, parallel and perpendicular relative to the pump beam with a polarizer. Both probe components are focused into an imaging spectrograph (SP2156 spectrograph, Princeton Instruments, 30 l/mm grating) and detected using a 128 × 128 pixel mercury cadmium telluride (MCT) array detector.
Frequency resolution on the pump axis is obtained in time domain, using the pulse shaper to generate two pump pulses delayed by 0 to 2555 fs at increments of 35 fs. To reduce data acquisition time we used a rotating frame at 1400 cm−1. Pump pulses were corrected for group-velocity dispersion, and the dispersion parameters were optimized using the transient signal generated from multi-photon absorption in a 0.5 mm thick Ge plate. Before transforming the thus determined free induction decays into the frequency domain, the time-domain data were zero-padded to 128 data points and filtered with a Hamming window.
For DRS experiments, 1 mL of each sample was brought in contact with the coaxial probes. For NMR experiments, 0.5 mL of the samples were placed in an NMR tube together with a capillary filled with DMSO-d6 for referencing. For all infrared experiments, solutions were contained between two CaF2 windows (2 mm thickness, 2.54 cm diameter) separated by a 25 µm Teflon spacer. The infrared absorption spectra were measured right before collecting the 2D-IR data.
Most recents protocols related to «Alanylalanine»
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Focusing on the carbohydrate metabolism associated metabolites, the study reported lowering of simple sugars in BV+ environment, and the same is observed in our results too; maltose being one of them, that overlap with them and follow the correct trend. Also, glucose-6-phosphate, and sugar alcohols like sorbitol and mannitol are other reported carbohydrate metabolism metabolites that are correctly predicted and maintain the trend of being present in lower amounts in BV+ cases. The same explanation that justified our amino acids metabolite prediction could also justify the case for carbohydrate metabolism metabolites; while the simple sugars and intermediate metabolites are being used up, the carbohydrate catabolites tend to accumulate in BV+ samples with the growing diversity of microbes.
They also reported lowering of glycerol, ethanolamine and glycerophosphorylcholine (GPC), all of which are associated with lipid metabolism, in BV+ samples and they too were correctly predicted.
In the spectrometer, a weak reflection90 (link),91 (link) from a wedged ZnSe window is used as probe beam. The transmitted IR light is guided to a pulse shaper, where it is diffracted from a grating (150 l/mm), collimated using a parabolic mirror, and guided to a Germanium-based acousto-optic modulator (AOM). The IR light is diffracted at the AOM and focused onto a second grating (150 l/mm). The shaped beam is reflected from a retroreflector on a translational stage to control the waiting time (T2) between the pump and the probe beams. After setting the polarization of the pump beam to 45° relative to the probe beam polarization, the pump and the probe beams are focused into the sample using an off-axis parabolic mirror. After the sample, the probe beam is re-collimated and split into polarization components, parallel and perpendicular relative to the pump beam with a polarizer. Both probe components are focused into an imaging spectrograph (SP2156 spectrograph, Princeton Instruments, 30 l/mm grating) and detected using a 128 × 128 pixel mercury cadmium telluride (MCT) array detector.
Frequency resolution on the pump axis is obtained in time domain, using the pulse shaper to generate two pump pulses delayed by 0 to 2555 fs at increments of 35 fs. To reduce data acquisition time we used a rotating frame at 1400 cm−1. Pump pulses were corrected for group-velocity dispersion, and the dispersion parameters were optimized using the transient signal generated from multi-photon absorption in a 0.5 mm thick Ge plate. Before transforming the thus determined free induction decays into the frequency domain, the time-domain data were zero-padded to 128 data points and filtered with a Hamming window.