75 research outputs found
T cells from the brain of <i>Il21</i><sup>−/−</sup> mice produce less IFN-γ during chronic toxoplasmic encephalitis.
<p>A) Flow cytometry of BMNCs from WT and <i>Il21</i><sup>−/−</sup> mice infected for 35 days; cells were stimulated <i>ex vivo</i> with PMA and ionomycin in the presence of brefeldin A for 4 h and then stained intracellularly for IFN-γ. Numbers in boxed areas represent percent IFN-γ<sup>+</sup> CD4<sup>+</sup> (left) or CD8<sup>+</sup> (right) T cells, while bold numbers indicate MFI. B) Total IFN-γ<sup>+</sup>CD4<sup>+</sup> or CD8<sup>+</sup> T cells isolated from BMNC preparations of WT (black bars) and <i>Il21</i><sup>−/−</sup> (white bars) mice infected for 35 days, calculated from the percentages determined by flow cytometry. Data are representative of four independent experiments with similar results. Error bars represent SEM. Significance was determined by a two-tailed unpaired Student’s <i>t</i> test. **<i>P</i><0.01.</p
Relationship Between Molecular Contact Thermodynamics and Surface Contact Mechanics
Measurements have been made of the adhesion and friction
forces
between organic monolayers in heptane/acetone mixtures using an atomic
force microscope (AFM). It has been found that the contact mechanics
are best modeled by treating the friction force as the sum of a load-dependent
term (attributed to “molecular plowing”) and an area-dependent
term attributed to shearing (adhesion). The relative contributions
of plowing and shearing are determined by the coefficient of friction,
μ, and the surface shear strength τ. The transition from
adhesion- to load-determined friction is controlled by the solvation
state of the surface: solvated surfaces represent a limiting case
in which the shear term approaches zero, and the friction-load relationship
is linear, while in other circumstances, the friction-load relationship
is nonlinear and consistent with Derjaguin–Muller–Toporov
mechanics. A striking correlation has been observed between the concentration-dependence
of the association constant (<i>K</i><sub>a</sub>) for the
formation of 1:1 hydrogen-bonded complexes and the pull-off force <i>F</i><sub>a</sub> and surface shear strength τ for the
same molecules when one partner is immobilized by attachment to an
AFM probe and the other is adsorbed to a surface. Analysis of the
concentration-dependence of <i>F</i><sub>a</sub> and τ
enables the prediction of <i>K</i><sub>S</sub> with remarkably
high precision, indicating that for these hydrogen bonding systems,
the tip–sample adhesion is dominated by the H-bond thermodynamics.
For mixed monolayers, H-bond thermodynamics dominate the interaction
even at very low concentrations of the H-bond acceptor. Even for weakly
adhering systems, a nonlinear friction-load relationship results.
The variation in τ with the film composition is correlated very
closely with the variation in <i>F</i><sub>a</sub>. However,
the coefficient of friction varies little with the film composition
and is invariant with the strength of tip–sample adhesion,
being dominated by molecular plowing and, for sufficiently large concentrations
of hydroxyl terminated adsorbates, the disruption of intramonolayer
hydrogen bonding interactions
<i>Il21</i><sup>−/−</sup> mice have reduced inflammatory cell numbers in the brain during chronic <i>T. gondii</i> infection.
<p>A) The percentage of CD4<sup>+</sup> (left) and CD8<sup>+</sup> (right) T cells expressing the cytokine IL-10 in the brain of individual WT and <i>Il21</i><sup>−/−</sup> mice infected for 35 days. Data are representative of two or three independent experiments with three to four mice per group. B) Enumeration of total cell numbers recovered from the brain of WT and <i>Il21</i><sup>−/−</sup> mice infected for 35 days. Data are representative of three experiments with similar results. C) Total CD4<sup>+</sup> T cells, CD8<sup>+</sup> T cells, macrophages and microglia in each BMNC preparation from (B), calculated by the percentages determined by flow cytometry. D) Total IL-10<sup>+</sup> CD4<sup>+</sup> and CD8<sup>+</sup> T cells in each BMNC preparation from (A), calculated by the percentages determined by flow cytometry. E) Flow cytometry of CD4<sup>+</sup> T cells isolated from WT and <i>Il21</i><sup>−/−</sup> mice, and activated with anti-CD3 and anti-CD28 in cRPMI (left) or IMDM (right) media in the presence of IL-27 for 4 days. Cells were then stimulated for 4 h with PMA and ionomycin in the presence of brefeldin A before staining for intracellular IL-10. Numbers in boxed areas indicate percent IL-10<sup>+</sup>CD4<sup>+</sup> T cells. Results are representative of three independent experiments with similar results. Significance was determined by a two-tailed unpaired Student’s <i>t</i> test. Error bars represent SEM. *<i>P</i><0.05, **<i>P</i><0.01.</p
<i>Il21</i><sup>−/−</sup> mice have an impaired antibody-mediated immune response during chronic toxoplasmic encephalitis.
<p>A) ELISA of IgM, IgG and IgG2c STAg-specific Ab titers in the serum of WT and <i>Il21</i><sup>−/−</sup> mice infected for 56 days. B, C) Flow cytometry of splenocytes isolated from day 35 infected WT or <i>Il21</i><sup>−/−</sup> mice and stained for (B) germinal center (GC) B cells (CD19<sup>+</sup>B220<sup>+</sup>PNA<sup>+</sup>) or (C) T<sub>FH</sub> cells (CD4<sup>+</sup>ICOS<sup>+</sup>CXCR5<sup>+</sup>). Numbers in the box represent the percent of (B) PNA<sup>+</sup>CD19<sup>+</sup> B cells or (C) CD4<sup>+</sup>ICOS<sup>+</sup>CXCR5<sup>+</sup> T<sub>FH</sub> cells. Quantitation of (B) GC B cells, or (C) T<sub>FH</sub> cells on day 35 and 56 p.i. from the spleen of WT and <i>Il21</i><sup>−/−</sup> mice. Error bars represent SEM. Data are representative of two (A) or three (B, C) independent experiments with similar results.</p
Relationship between Chemical Structure and Supramolecular Effective Molarity for Formation of Intramolecular H‑Bonds
Effective molarity
(EM) is a key parameter that determines the
efficiency of a range of supramolecular phenomena from the folding
of macromolecules to multivalent ligand binding. Coordination complexes
formed between zinc porphyrins equipped H-bond donor sites and pyridine
ligands equipped with H-bond acceptor sites have allowed systematic
quantification of EM values for the formation of intramolecular H-bonds
in 240 different systems. The results provide insights into the relationship
of EM to supramolecular architecture, H-bond strength, and solvent.
Previous studies on ligands equipped with phosphonate diester and
ether H-bond acceptors were inconclusive, but the experiments described
here on ligands equipped with phosphine oxide, amide, and ester H-bond
acceptors resolve these ambiguities. Chemical double-mutant cycles
were used to dissect the thermodynamic contributions of individual
H-bond interactions to the overall stabilities of the complexes and
hence determine the values of EM, which fall in the range 1–1000
mM. Solvent has little effect on EM, and the values measured in toluene
and 1,1,2,2-tetrachloroethane are similar. For H-bond acceptors that
have similar geometries but different H-bond strengths (amide and
ester), the values of EM are very similar. For H-bond acceptors that
have different geometries but similar H-bond strengths (amide and
phosphonate diester), there is little correlation between the values
of EM. These results imply that supramolecular EMs are independent
of solvent and intrinsic H-bond strength but depend on supramolecular
architecture and geometric complementarity
Metal Hydrides Form Halogen Bonds: Measurement of Energetics of Binding
The
formation of halogen bonds from iodopentafluorobenzene and
1-iodoperfluorohexane to a series of bis(η<sup>5</sup>-cyclopentadienyl)metal
hydrides (Cp<sub>2</sub>TaH<sub>3</sub>, <b>1</b>; Cp<sub>2</sub>MH<sub>2</sub>, M = Mo, <b>2</b>, M = W, <b>3</b>; Cp<sub>2</sub>ReH, <b>4</b>; Cp<sub>2</sub>Ta(H)CO, <b>5</b>; Cp = η<sup>5</sup>-cyclopentadienyl) is demonstrated by <sup>1</sup>H NMR spectroscopy. Interaction enthalpies and entropies for
complex <b>1</b> with C<sub>6</sub>F<sub>5</sub>I and C<sub>6</sub>F<sub>13</sub>I are reported (Δ<i>H</i>°
= −10.9 ± 0.4 and −11.8 ± 0.3 kJ/mol; Δ<i>S</i>° = −38 ± 2 and −34 ± 2 J/(mol·K),
respectively) and found to be stronger than those for <b>1</b> with the hydrogen-bond donor indole (Δ<i>H</i>°
= −7.3 ± 0.1 kJ/mol, Δ<i>S</i>° =
−24 ± 1 J/(mol·K)). For the more reactive complexes <b>2</b>–<b>5</b>, measurements are limited to determination
of their low-temperature (212 K) association constants with C<sub>6</sub>F<sub>5</sub>I as 2.9 ± 0.2, 2.5 ± 0.1, <1.5,
and 12.5 ± 0.3 M<sup>–1</sup>, respectively
Validation of a Computational Cocrystal Prediction Tool: Comparison of Virtual and Experimental Cocrystal Screening Results
A virtual cocrystal screening method
based on calculated gas phase
molecular electrostatic potential surfaces (MEPS) of the individual
components has been validated using experimental cocrystal screens
reported in the literature. The noncovalent interactions of a molecule
with its environment are described by a discrete set of independent
surface site interaction points (SSIPs), whose properties can be calculated
from the <i>ab initio</i> MEPS. The stability of a crystal
is estimated based on pairing SSIPs such that the sum of the pairwise
interaction energies is optimized. This provides a means of calculating
the relative stability of a cocrystal compared with the pure components
without knowing anything about the three-dimensional structures of
the crystalline states. For a set of potential crystal coformers (CCF),
the difference between interaction site pairing energies of different
solid forms (Δ<i>E</i>) provides a method for ranking
CCFs based on the calculated probability of cocrystal formation. The
method was applied to cocrystal screens of 18 compounds that reported
both hits and misses, and in most cases, the virtual cocrystal screen
reproduces experimental results well. In lists of CCFs ranked by Δ<i>E</i>, the experimentally observed hits were significantly enriched
at the top, and this indicates that virtual screening is a promising
tool for focusing experimental efforts on the most promising CCF candidates
Disruption of <i>TgPHIL1</i> Alters Specific Parameters of <i>Toxoplasma gondii</i> Motility Measured in a Quantitative, Three-Dimensional Live Motility Assay
<div><p><i>T. gondii</i> uses substrate-dependent gliding motility to invade cells of its hosts, egress from these cells at the end of its lytic cycle and disseminate through the host organism during infection. The ability of the parasite to move is therefore critical for its virulence. <i>T. gondii</i> engages in three distinct types of gliding motility on coated two-dimensional surfaces: twirling, circular gliding and helical gliding. We show here that motility in a three-dimensional Matrigel-based environment is strikingly different, in that all parasites move in irregular corkscrew-like trajectories. Methods developed for quantitative analysis of motility parameters along the smoothed trajectories demonstrate a complex but periodic pattern of motility with mean and maximum velocities of 0.58±0.07 µm/s and 2.01±0.17 µm/s, respectively. To test how a change in the parasite's crescent shape might affect trajectory parameters, we compared the motility of Δ<i>phil1</i> parasites, which are shorter and wider than wild type, to the corresponding parental and complemented lines. Although comparable percentages of parasites were moving for all three lines, the Δ<i>phil1</i> mutant exhibited significantly decreased trajectory lengths and mean and maximum velocities compared to the parental parasite line. These effects were either partially or fully restored upon complementation of the Δ<i>phil1</i> mutant. These results show that alterations in morphology may have a significant impact on <i>T. gondii</i> motility in an extracellular matrix-like environment, provide a possible explanation for the decreased fitness of Δ<i>phil1</i> parasites <i>in vivo</i>, and demonstrate the utility of the quantitative three-dimensional assay for studying parasite motility.</p></div
3D motility of the Δ<i>phil1</i> parasites.
<p>(<b>A</b>) MIPs for wild-type (RH), <i>TgPHIL1</i> knockout (Δ<i>phil1</i>) and complemented (Comp) parasites. Scale bar = 50 µm. The colour scheme for all MIPs was inverted for better visualization of parasite trajectories. The percentage of total parasites moving (<b>B</b>) was comparable for the three parasite lines, but the cumulative frequency distribution (<b>C</b>) and histogram (<b>D</b>) of the smoothed trajectory lengths for RH (black), Δ<i>phil1</i> (red) and Comp parasites (grey) reveal that the Δ<i>phil1</i> parasites do not move as far as the RH or Comp parasites within the same timeframe (Kolmogorov-Smirnov test, D = 0.199, p<0.0001 and D = 0.114, p<0.0001, respectively). The Δ<i>phil1</i> parasites also exhibited significantly decreased mean velocity compared to the RH parasites (<b>E</b>) and significantly reduced maximum velocity compared to both RH and Comp parasites (<b>F</b>) (paired t-test, significance indicated by asterisks). Closed data points are the results from five independent experiments comparing RH and Δ<i>phil1</i> parasites; open data points are the results from four independent experiments comparing Δ<i>phil1</i> and Comp parasites. Each of the independent experiments (assigned a different colour in the scatter plot) was performed in either triplicate or quadruplicate. The total number of parasites analyzed was 6,467 for RH, 9,305 for Δ<i>phil1</i> and 3,743 for Comp. * p<0.05, ** p<0.001, ns = not significant.</p
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