275 research outputs found
Signalling and Regulation of the Glucagon-like Peptide-1 receptor
Following nutrient ingestion, glucagon-like peptide 1 (GLP-1) secreted from intestinal L-cells mediates anti-diabetic effects, most notably stimulating glucose-dependent insulin release from pancreatic ÎČ-cells but also inhibiting glucagon release, promoting satiety and weight reduction and potentially enhancing or preserving ÎČ-cell mass. These effects are through the GLP-1 receptor (GLP-1R) which is a therapeutic target in type 2 diabetes. The present study focused on desensitisation and re-sensitisation of GLP-1R-mediated signalling and interactions of orthosteric and allosteric ligands. Data demonstrate GLP-1R desensitisation and subsequent re-sensitisation following removal of extracellular ligand with ligand-specific features. Following GLP-1-mediated desensitisation, re-sensitisation is dependent on receptor internalisation, endosomal acidification and receptor recycling. Re-sensitisation is also dependent on endothelin converting enzyme-1 (ECE-1) activity, possibly through proteolysis of GLP-1 in endosomes, facilitating disassociation of receptor-ÎČ-arrestin complexes leading to GLP-1R recycling and re-sensitisation. ECE-1 activity also regulates GLP-1-induced activation of extracellular signal regulated kinase (ERK) and generation of cAMP possibly through a G protein independent/ÎČ-arrestin dependent mechanism. By contrast, following GLP-1R activation by the orthosteric agonist, exendin-4, or allosteric agonist, compound 2, re-sensitisation was slow and independent of ECE-1 activity. Thus, different ligands depend on different events during GLP-1R trafficking which could be important for re-sensitisation and signalling, particularly that mediated by scaffolding around ÎČ-arrestin.
As the GLP-1R is targeted therapeutically at orthosteric and allosteric sites, this study examined activation of the GLP-1R by orthosteric and allosteric agonists and in particular interactions between ligands of these sites. Challenging the GLP-1R with the allosteric ligand, compound 2, along with GLP-1 9-36 amide, a low affinity, low efficacy metabolite of GLP-1 7-36 amide, results in synergistic receptor activation. This may be important for therapeutic approaches with allosteric ligands, as metabolites of GLP-1 may be present in vivo at concentrations higher than the classic endogenous ligand. Indeed this could present a novel therapeutic approach
Theoretical Insight into CoreâShell Preference for Bimetallic PtâM (M = Ru, Rh, Os, and Ir) Cluster and Its Electronic Structure
Pt<sub><i>m</i></sub>M<sub><i>n</i></sub> (M
= Ru, Rh, Os, and Ir; <i>m</i>+<i>n</i> = 38 and
55) clusters are systematically investigated using the DFT method.
In an octahedral 38-atom cluster, coreâshell structure M<sub>6</sub>@- Pt<sub>32</sub> with M<sub>6</sub> core and Pt<sub>32</sub> shell is stable for PtâRh and PtâIr combinations but
is not for PtâRu and PtâOs combinations. In a 55-atom
cluster, icosahedral M<sub>13</sub>@Pt<sub>42</sub> structure is stable
for all Pt-M combinations, indicating that a large cluster is more
preferable to stabilizing the coreâshell structure than a small
cluster. The difference in cohesive energy (<i>E</i><sub>coh</sub>) between M<sub>13</sub> and Pt<sub>13</sub> and the distortion
energy {<i>E</i><sub>dis</sub>(M<sub>13</sub>)} of M<sub>13</sub> are parallel to the segregation energy (<i>E</i><sub>seg</sub>), indicating that these are important factors for
stabilizing M<sub>13</sub>@Pt<sub>42</sub>. One more crucially important
factor is the interaction energy (<i>E</i><sub>int</sub>) between M<sub>13</sub> core and Pt<sub>42</sub> shell, because <i>E</i><sub>int</sub> is parallel to <i>E</i><sub>seg</sub> and its absolute value is much larger than those of <i>E</i><sub>dis</sub>(M<sub>13</sub>) and <i>E</i><sub>dis</sub>(Pt<sub>42</sub>). The <i>E</i><sub>int</sub> depends on
the energy gap between LUMO of M<sub>13</sub> core and HOMO of Pt<sub>42</sub> shell, indicating that LUMO energy of M<sub>13</sub> and
HOMO energy of Pt<sub>42</sub> are good properties for understanding
and predicting stability of coreâshell structure. Pt atom is
more positively charged in M<sub>13</sub>@Pt<sub>42</sub> than in
Pt<sub>55</sub> and the HOMO energy of M<sub>13</sub>@Pt<sub>42</sub> is higher than that of Pt<sub>55</sub>. The presence of these two
contrary factors for O<sub>2</sub> binding suggests that M<sub>13</sub>@Pt<sub>42</sub> is not bad for O<sub>2</sub> binding
Theoretical Insight into CoreâShell Preference for Bimetallic PtâM (M = Ru, Rh, Os, and Ir) Cluster and Its Electronic Structure
Pt<sub><i>m</i></sub>M<sub><i>n</i></sub> (M
= Ru, Rh, Os, and Ir; <i>m</i>+<i>n</i> = 38 and
55) clusters are systematically investigated using the DFT method.
In an octahedral 38-atom cluster, coreâshell structure M<sub>6</sub>@- Pt<sub>32</sub> with M<sub>6</sub> core and Pt<sub>32</sub> shell is stable for PtâRh and PtâIr combinations but
is not for PtâRu and PtâOs combinations. In a 55-atom
cluster, icosahedral M<sub>13</sub>@Pt<sub>42</sub> structure is stable
for all Pt-M combinations, indicating that a large cluster is more
preferable to stabilizing the coreâshell structure than a small
cluster. The difference in cohesive energy (<i>E</i><sub>coh</sub>) between M<sub>13</sub> and Pt<sub>13</sub> and the distortion
energy {<i>E</i><sub>dis</sub>(M<sub>13</sub>)} of M<sub>13</sub> are parallel to the segregation energy (<i>E</i><sub>seg</sub>), indicating that these are important factors for
stabilizing M<sub>13</sub>@Pt<sub>42</sub>. One more crucially important
factor is the interaction energy (<i>E</i><sub>int</sub>) between M<sub>13</sub> core and Pt<sub>42</sub> shell, because <i>E</i><sub>int</sub> is parallel to <i>E</i><sub>seg</sub> and its absolute value is much larger than those of <i>E</i><sub>dis</sub>(M<sub>13</sub>) and <i>E</i><sub>dis</sub>(Pt<sub>42</sub>). The <i>E</i><sub>int</sub> depends on
the energy gap between LUMO of M<sub>13</sub> core and HOMO of Pt<sub>42</sub> shell, indicating that LUMO energy of M<sub>13</sub> and
HOMO energy of Pt<sub>42</sub> are good properties for understanding
and predicting stability of coreâshell structure. Pt atom is
more positively charged in M<sub>13</sub>@Pt<sub>42</sub> than in
Pt<sub>55</sub> and the HOMO energy of M<sub>13</sub>@Pt<sub>42</sub> is higher than that of Pt<sub>55</sub>. The presence of these two
contrary factors for O<sub>2</sub> binding suggests that M<sub>13</sub>@Pt<sub>42</sub> is not bad for O<sub>2</sub> binding
Functional interaction between ligands on GLP-1R-mediated cAMP generation in HEK-GLP-1R cells.
<p>HEK-GLP-1R cells were pretreated (Pre-) for 10 min with 1 ”M GLP-1 9â36 amide in the presence of IBMX before challenge for 15 min with the indicated concentrations of agonists. Where no pre-treatment is indicated, an equivalent volume of buffer (KHB) was added for 10 min in the presence of IBMX prior to ligand addition for 15 min. Levels of intracellular cAMP were then determined relative to the cellular protein content. The final concentration of DMSO (vehicle) for the 15 min treatment period was 5% v/v in all cases. Data are mean±s.e.m., nâ=â3.</p
Time course of cAMP generation in response to GLP-1 9â36 amide, compound 2 or co-stimulation in HEK-GLP-1R cells.
<p>HEK-GLP-1R cells were either untreated (Basal; not visible) or treated for the indicated times with GLP-1 9â36 amide (1 ”M), compound 2 (1 ”M) or the two in combination (Co-addition) in the presence of IBMX. The final concentration of DMSO (vehicle) was 5% v/v in all cases. In addition to the measured levels of cAMP generation, the numerical sum of cAMP generation in response to GLP-1 9â36 amide and compound 2 alone are presented (Numerical). Data are mean±s.e.m., nâ=â3, ** P<0.01 and *** P<0.001 by Bonferroni's multiple range test following oneway ANOVA. For clarity, only differences between ânumericalâ and âco-additionâ conditions are shown.</p
High Molecular Weight Polyesters Derived from Biobased 1,5-Pentanediol and a Variety of Aliphatic Diacids: Synthesis, Characterization, and Thermo-Mechanical Properties
High molecular weight
aliphatic polyesters were synthesized from
biobased 1,5-pentanediol and aliphatic diacids with 4, 5, 6, 9, 10,
or 12 carbon atoms via melt polycondensation. The polyÂ(1,5-pentylene
dicarboxylate)Âs were characterized with intrinsic viscosity, gel permeation
chromatography (GPC), nuclear magnetic resonance (NMR), differential
scanning calorimetry (DSC), wide-angle X-ray diffraction (WAXD), thermogravimetric
analysis (TGA), and tensile testing. The effects of dicarboxylate
chain length on crystalline structure and thermo-mechanical properties
were investigated. All the polyesters had weight-average molecular
weight over 100,000 g/mol or intrinsic viscosity over 1.05 dL/g except
polyÂ(1,5-pentylene adipate) (PPeA), which was less thermally stable
than others. As semicrystalline polymers, they have a polyethylene-like
crystal structure and crystallize rapidly except polyÂ(1,5-pentylene
succinate) (PPeS). As a whole, the crystallizability and melting temperature
(<i>T</i><sub>m</sub>) increase with dicarboxylate chain
length, and the âevenâoddâ effect exists to a
certain extent. Among them, polyÂ(1,5-pentylene azelate) (PPeAz), polyÂ(1,5-pentylene
sebacate) (PPeSe), and polyÂ(1,5-pentylene dodecanedioate) (PPeDo)
have <i>T</i><sub>m</sub> of 50â62 °C, good
thermal stability, and exhibit comparable or even superior tensile
properties in comparison with polyethylene and the well-known biodegradable
copolyester, polyÂ(butylene adipate-<i>co</i>-terephthalate)
(PBAT). These biobased and potentially biodegradable polyesters appear
to be promising materials for practical applications
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