Because of the thin HIPed walls of the channels, the specimen size for inspection of HIPed interface is limited.
The sequence of structural transformations at the Ti/Al interface is limited by the reaction temperature and time.
This way, a large amount of carbon atoms are incorporated into substitutional sites and the migration of mobile carbon atoms to the Si cap/SiO2 interface is limited.
In addition, the variation of mechanical properties of this system as a function of Co indicates that the interfacial pressure jump can be significantly larger when the bulk transport of surfactant to the interface is limited.
The propagation range of SPPs on a metal-dielectric interface is limited due to ohmic losses and scattering on random and intended interface irregularities [2 4].
The application of such an interface is limited to people with sufficient head motion that is able to reach the joystick.
In each mobile system with a dispersion of the signal spectrum, the capacity of the radio interface is limited following an occurrence of a number of types of interference noise, most notably interference from users being serviced in neighboring cells.
Because of the difficulty in determining accurate seismic velocities for the deeper lithologies, information on the location of the décollement and back-stop interface is limited along seismic lines MY103 and BS101.
Under these conditions, the hole supply to the interface is limited by the transport across the space charge region (SCR), making the analogy with the n-Si case rather straightforward.
However, this interface is limited to small- to medium-scale queries, and text mining using this interface is not possible.
