Accordingly, a primary goal of this paper is identify the circumstances under which measurable cost saving can be achieved when one aircraft transports a request from its origin to an intermediate point and a second aircraft picks it up and delivers it to its final destination.
One major concern with such projects, however, is that the evolutionary pathway may be highly substrate-specific, and it can be difficult to follow a path that encounters a dead end at an intermediate point.
This path demonstrates the characteristic pattern of gains and losses of a zigzag path: before each CD step, SD steps in the opposite direction are inserted to prevent the path from having an intermediate point with a more extreme copy number than the endpoint of the path.
Free flexural vibrations of vertical rods having an attached mass at an intermediate point and different end constraints are investigated, with consideration of the axial force owing to the weight of a mass.
The layout of the facility is fixed, the edges on the boundary of the manufacturing cells are candidates to form the unidirectional loop flow path, and a set of nodes located at an intermediate point on each edge are candidates for pickup and delivery stations of the cell formed by those edges.
This paper considers the stabilization of a second order ODE heat system coupling at an intermediate point under natural and checkable assumptions, which is motivated by the thermoelastic coupling physics arising in microelectromechanical systems (MEMS).
A portable electromagnetic field meter measured the field strength of the radar at three distances from the source: in close proximity (<200 m) with a high electromagnetic field (EMF) strength >2 volts/metre, an intermediate point within line of sight of the radar (200 400 m) and with an EMF strength <2 v/m, and a control site out of sight of the radar (>400 m) and registering an EMF of zero v/m.
Furthermore, the given boundary conditions are also interesting and important from a physical point of view [15, 16] as the condition D δ x ( 1 ) − D δ x = a is a fractional analogue of the classical flux condition x ′ ( 1 ) − x ′ = a (the difference of flux values at the right end point and at an intermediate point of the interval [ 0, 1 ] remains constant).
This note is concerned with the vibrations of a beam carrying a concentrated mass at the beam tip and another concentrated mass at an intermediate point.
The problem of a cable with bending stiffness, attached with both lateral and rotational dampers at an intermediate point, is therefore considered in this study.
