1,431 Works
Rapid mechanical stimulation of inner-ear hair cells by photonic pressure
Sanjeewa Abeytunge, Francesco Gianoli, A. James Hudspeth & Andrei S. Kozlov
Hair cells, the receptors of the inner ear, detect sounds by transducing mechanical vibrations into electrical signals. From the top surface of each hair cell protrudes a mechanical antenna, the hair bundle, which the cell uses to detect and amplify auditory stimuli, thus sharpening frequency selectivity and providing a broad dynamic range. Current methods for mechanically stimulating hair bundles are too slow to encompass the frequency range of mammalian hearing and are plagued by inconsistencies....
Section 5 NTOs
Zoe Jeffers
The log and fchk files for NTOs in Section 5. Contains NTOs for the first and second singlet excited state of 6C, 7C, 13C, and 14C, and the first excited state of 10 and 11E. Calculated using wB97XD/DGTZVP from wB97XD/DGTZVP excited state checkpoint files.
1-cyclopentyl-3-(2-isopropyl-5-methylphenoxy)propan-2-one
Lu Qian
0.749 g of thymol and 0.714 g of Cyclopentylacetic acid was measured out. In a round bottom flask with a magnetic stirrer bar, 15mL of acetonitrile, 0.5 mmol of DMAP and 6.5 mmol of EDC·HCl was added. Then the acid and thymol were added add with the aid of acetonitrile (10 mL) each. Heater and stirring was turned on after the condenser was set to run (100 °C). TLC assessments were carried out every hour...
Et TS2 (12)
Natnicha Limpaitoon
TS2, b3lyp+GD3BJ/Def2-SVPP, SCRF=THF, ΔG = -1634.1805 ΔΔG = 4.71
Data for drainage capillary pressure distribution and fluid displacement in a heterogeneous laminated sandstone
Qingyang Lin, Branko Bijeljic & Martin Blunt
We applied three-dimensional X-ray microtomography to image a capillary drainage process (0-1000 kPa) in a cm-scale heterogeneous laminated sandstone containing three distinct regions with different pore sizes to study the capillary pressure. We used differential imaging to distinguish solid, macro pore and five levels of sub-resolution pore phases associated with each region. The brine saturation distribution was computed based on average CT values. The non-wetting phase displaced the wetting phase in order of pore size...
TISQOE W-N (-1)
Henry Rzepa
Gaussian Calculation
TISQOE Ru-N(+)
Henry Rzepa
Gaussian Calculation
Fe(-)C trigonal, quad pinned back, triple
Henry Rzepa
Gaussian Calculation
iPr TS2 (2 Me rotated towards Ad) (13)
Natnicha Limpaitoon
TS2, b3lyp+GD3BJ/Def2-SVPP, SCRF=THF, ΔG = -1673.4412 ΔΔG = 6.77
GAJXOH
Henry Rzepa
Gaussian Calculation
MeF2I-CC reactant, Def2-TZVPPD, G = -613.357322
Henry Rzepa
Gaussian Calculation
Py-CC 1,2-dimerisation, Def2-TZVPPD, G = -648.526431
Henry Rzepa
Gaussian Calculation
Data from: Gravity and active acceleration limit the ability of killer flies (Coenosia attenuata) to steer towards prey when attacking from above
Sergio Rossoni, Samuel Fabian, Gregory Sutton & Paloma Gonzalez-Bellido
Insects that predate aerially usually contrast prey against the sky and attack upwards. However, killer flies (Coenosia attenuata) can attack prey flying below them, performing what we term 'aerial dives'. During these dives, killer flies accelerate up to 36 m/s2. Although the trajectories of the killer fly's dives appear highly variable, proportional navigation explains them, as long as the model has the lateral acceleration limit of a real killer fly. The trajectory's steepness is explained...
MeI-CC 1,2-dimerisation, Def2-TZVPPD, G = -827.345930
Henry Rzepa
Gaussian Calculation
Coordinates
Feriel Rekhroukh
DFT Coordinates
DFT coordinates
Feriel Rekhroukh
DFT coordinates
Spirit Checklist: Pharmacokinetics and Pharmacodynamics of azithromycin in severe malaria bacterial co-infection in African children (TABS-PKPD)
Kathryn Maitland
TABS PKPD Standard Protocol items For intervention trials Checklist and Assessment schedule
iPr TS3 (24)
Natnicha Limpaitoon
TS3, b3lyp+GD3BJ/Def2-SVPP, SCRF=THF, ΔG = -1441.4132, ΔΔG = 7.84
Cope amination IRC
Henry Rzepa
Gaussian Calculation
Cope amination Ph IRC
Henry Rzepa
Gaussian Calculation
1,3,5-trifluoromethylphenyl-I, G = -1539.272696
Henry Rzepa
Gaussian Calculation
Ph-Stevens, Reactant, 1,2 with retention \"forbidden\", RHF, Def2-SVP, water, G = -522.802526
Henry Rzepa
Gaussian Calculation
Ph-Stevens, 1,2 with inversion \"allowed\" UHF TS for C-N bond formation G = -522.799570
Henry Rzepa
Gaussian Calculation
Ph-Stevens, 1,2 Product
Henry Rzepa
Gaussian Calculation
PhICC + CCCCIPh, branched mode to produce C5 chain, syn G = -1286.086804 IRC
Henry Rzepa
Gaussian Calculation
Affiliations
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Imperial College London1,431
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Zhejiang University6
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University of Cambridge6
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Affiliated Hospital of Nantong University4
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Henan University4
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North West Agriculture and Forestry University4
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Sun Yat-sen University4
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West China Hospital of Sichuan University4
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University of Oxford4
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London School of Hygiene & Tropical Medicine3