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first mode
It has been shown that the middle regime is unstable, only the first mode of the small disturbances being unstable over a broad range of the parameters.
      
In the first mode, which is realized at rather substantial differences between the initial temperature of the reservoir and the temperature of water being injected, the condensation of steam occurs at the interface.
      
In the first mode, input processes are digitized after a START signal; in the second mode, a signal exceeding a preset threshold is uninterruptedly sought for and recorded.
      
These velocity deviations have been determined for the first mode of Love waves and for the zero mode of SH waves as functions of the thickness and acoustic properties of the coating and substrate.
      
It is shown that the frequency band of the received signal can be broadened by introducing a frequency-time correction of the propagation time of the first mode as a function of the sound frequency.
      
In addition to the signal with the directivity of the third mode, a signal is observed with the directivity of the first mode, which slightly advances the signal of the third mode but arrives noticeably later than the first-mode signal.
      
The frequency-dependent energy fluctuations of the signals and those of the first mode alone were measured in the frequency range 10-80 Hz.
      
It is shown that the amplitudes of energy fluctuations of the first mode in narrow bands can exceed 10 dB and make the main contribution to the energy fluctuations of the total signal.
      
The maximum energy of the first mode is reached on the high tide.
      
It is hypothesized that internal tide-induced variations of the sound velocity field on the shelf affect the degree of energy interaction between the first mode and the bottom.
      
A pressure-release bottom and a bottom with an impedance that is intermediate between the pressure-release and rigid cases correspond to the first mode and the higher modes, respectively.
      
It is shown for the first time that there exist two modes of nuclear multifragmentation, those where less (first mode) or more (second mode) than half of nucleons are knocked out of the incident nucleus.
      
It is shown that acceleration by combined radiation is more effective than acceleration by Gaussian beams of the lowest or the first mode.
      
The second mode corresponds to modulation of the fundamental (first) mode.
      
The first mode decays on a very-short-length scale (≈nm).
      
The first mode (EOF1) reveals variations of basin-wide thermocline depth, which is mainly caused by surface heating.
      
Though the most unstable T-S wave was of second mode for laminar flow, the first mode waves played the key role in the breakdown process in laminar-turbulent transition.
      
The linear stability theory was applied for the analysis of the first mode and the second mode unstable waves under both isothermal and adiabatic wall condition, and eN method was used for the prediction of transition location.
      
The results show that the mechanism of secondary instability does work, whether the 2-D fundamental disturbance is of the first mode or second mode T-S wave.
      
The analysis of disc-preserving mappings in a Lagrangian scheme provides the expression for the operator that generates the linear relations for the first mode and, by an extension, those found by Virasoro for all modes.
      
 

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