Electric Field Driven Torque in ATP Synthase Miller, J.H., Jr
... Figure 2 shows cross-sections of the resulting equipotential surfaces (black lines) and tangential electric field components (red arrows), superimposed on an idealized cross section of the c-ring (yellow) and a-subunit (green). The proton channel cross sections in the a-subunit are colored to depict ...
... Figure 2 shows cross-sections of the resulting equipotential surfaces (black lines) and tangential electric field components (red arrows), superimposed on an idealized cross section of the c-ring (yellow) and a-subunit (green). The proton channel cross sections in the a-subunit are colored to depict ...
Mechanics
... Another typical example is the bicycle (Fig. 1b). We can move more quickly on a bicycle than on foot. There are also other types of machines, which do not save energy or increase velocity, but are used to change directions of the applied forces conveniently. A fixed pulley is one of the typical exam ...
... Another typical example is the bicycle (Fig. 1b). We can move more quickly on a bicycle than on foot. There are also other types of machines, which do not save energy or increase velocity, but are used to change directions of the applied forces conveniently. A fixed pulley is one of the typical exam ...
Integral Vector Theorems
... (a) dS is a unit normal pointing outwards from the interior of the volume V . (b) Both sides of the equation are scalars. (c) The theorem is often a useful way of calculating a surface integral over a surface composed of several distinct parts (e.g. a cube). (d) ∇ · F is a scalar field representing ...
... (a) dS is a unit normal pointing outwards from the interior of the volume V . (b) Both sides of the equation are scalars. (c) The theorem is often a useful way of calculating a surface integral over a surface composed of several distinct parts (e.g. a cube). (d) ∇ · F is a scalar field representing ...
SELF-CONSISTENT SIMULATION OF RADIATION AND SPACE-CHARGE IN HIGH-BRIGHTNESS RELATIVISTIC ELECTRON BEAMS
... bunch charge is 0.3 nC, and the final rms pulse length is 0.2 ps. The offset in both coordinates is due to the net energy loss of the beam. The normalized rms emittance, which is corrected for the offsets in centroids, is 18.5 mm-mrad (initial was 2 mm-mrad). . . . . . . . . . 113 5.13 Longitudinal ...
... bunch charge is 0.3 nC, and the final rms pulse length is 0.2 ps. The offset in both coordinates is due to the net energy loss of the beam. The normalized rms emittance, which is corrected for the offsets in centroids, is 18.5 mm-mrad (initial was 2 mm-mrad). . . . . . . . . . 113 5.13 Longitudinal ...
Physics - Rwanda Education Board
... The Rwanda Education Board is honoured to provide syllabuses which serve as both official documents and as a guide to competence-based teaching and learning. These syllabuses ensure consistency and coherence in the delivery of quality education across all levels of general education in Rwandan schoo ...
... The Rwanda Education Board is honoured to provide syllabuses which serve as both official documents and as a guide to competence-based teaching and learning. These syllabuses ensure consistency and coherence in the delivery of quality education across all levels of general education in Rwandan schoo ...
The physics of fusion power
... The likelihood of a fusion reaction is expressed in terms of a cross-section. A cross section has the dimension of an area, and one can roughly think of it as the size of the particles. A snooker ball, for instance, would have a cross section πr2 where r is the radius of the ball. For a fusion react ...
... The likelihood of a fusion reaction is expressed in terms of a cross-section. A cross section has the dimension of an area, and one can roughly think of it as the size of the particles. A snooker ball, for instance, would have a cross section πr2 where r is the radius of the ball. For a fusion react ...