Interaction of the C-terminal peptide from pigeon cytochrome C with
... effect (+1) drives its interaction with the negatively charged environment surrounding the metal surface. The medium SERS band of the peptide at 728 cm-1, is assigned to a coupled vibration involving the ρCH2 and COO- deformation modes [6]. This band characterizes most of amino acids containing the ...
... effect (+1) drives its interaction with the negatively charged environment surrounding the metal surface. The medium SERS band of the peptide at 728 cm-1, is assigned to a coupled vibration involving the ρCH2 and COO- deformation modes [6]. This band characterizes most of amino acids containing the ...
Contamination profile of Printed Circuit Board Assemblies in relation
... left on the top of the PCBA, through via-holes, and the difference in the temperature of the top and bottom parts of the PCBA during soldering could introduce higher amounts of residue on the top part, where the temperature reaches only up to 170 ºC (Figure 3 a and b). In the case of selective wave ...
... left on the top of the PCBA, through via-holes, and the difference in the temperature of the top and bottom parts of the PCBA during soldering could introduce higher amounts of residue on the top part, where the temperature reaches only up to 170 ºC (Figure 3 a and b). In the case of selective wave ...
Induced nanoscale deformations in polymers using atomic
... value k ⬇ 0.9 produces an electric field inside a polymer film of the order of 108 – 109 V m−1,17 well below the electric breakdown threshold. Equation (9) presents an averaged field instead of Ein共r兲 or Eout共r兲 excluding self-action.13 The expression has two components for tensile 共T⬜兲 and shear 共T ...
... value k ⬇ 0.9 produces an electric field inside a polymer film of the order of 108 – 109 V m−1,17 well below the electric breakdown threshold. Equation (9) presents an averaged field instead of Ein共r兲 or Eout共r兲 excluding self-action.13 The expression has two components for tensile 共T⬜兲 and shear 共T ...
Pore Scale Modeling of Rock Properties and Comparison to Laboratory Measurements
... conductivity value σ of a composite n-phase material is a function of location r. For steady state conductivity problems, where the currents are steady in time, the charge conservation equation possesses the same form as the Laplace equation. Between phases having different conductivities, ...
... conductivity value σ of a composite n-phase material is a function of location r. For steady state conductivity problems, where the currents are steady in time, the charge conservation equation possesses the same form as the Laplace equation. Between phases having different conductivities, ...
Stabilization of Rock Salt ZnO Nanocrystals by Low
... ZnO and MgO Surface Energies. The DFT calculations on bulk formation energies suggest that, even at finite temperature, RS MgxZn1−xO is stable for only small amounts of Zn. Therefore, this effect is not sufficient to explain the rock salt phase found experimentally in Mg-doped ZnO nanocrystals, whereby ...
... ZnO and MgO Surface Energies. The DFT calculations on bulk formation energies suggest that, even at finite temperature, RS MgxZn1−xO is stable for only small amounts of Zn. Therefore, this effect is not sufficient to explain the rock salt phase found experimentally in Mg-doped ZnO nanocrystals, whereby ...
Ultrahydrophobicity
Superhydrophobic surfaces are highly hydrophobic, i.e., extremely difficult to wet. The contact angles of a water droplet exceeds 150° and the roll-off angle/contact angle hysteresis is less than 10°. This is also referred to as the Lotus effect, after the superhydrophobic leaves of the lotus plant. Droplet impacting on these kind of surfaces can fully rebound like an elastic ball, or pancake.