This system is called MBS (Electro-Magnetic Induction Blasting System), which is based on Faraday Electro-Magnetic Induction Principle together with the frequency transmitting feature of the soft Mn-Zn ferrite as shown in Fig.

The plane wave transmission properties of a Y slotted array backed with multilayer dielectric are studied in this paper. The mode matching techniques for solving the frequencyresponse of this kind of FSS structure is introduced, and the influence of dielectric thickness on theresonance frequency, transmission loss, as well as the.

An analysis is made of the influence of defects on the averaged Green's function of optical phonons whose imaginary part is proportional to the cross section for Raman one-phonon light scattering, which depends on the frequency transfer.

The differences from independent time-transfer techniques such as TWSTFT (two-way satellite time and frequency transfer) are a few nanoseconds for both products.

Furthermore, high-frequency transfer of plasmid RP4 fromC.

Frequency transfer properties of three distinct types of cat horizontal cells

Frequency transfer functions are presented for the three types of H-units and a phenomenological model is discussed that describes these results quantitatively.

On the possibility of soliton-like double-frequency propagation of femtosecond pulses in an optical fiber under conditions of se

A soliton-like mode of double-frequency propagation of femtosecond pulses during second harmonic generation (SHG) in optical fibers is predicted on the basis of computer simulation.

Effect of time scale synchronization on the accuracy of very-low frequency propagation phase velocity measurement

Low-Frequency Propagation of Plane Scalar Waves through a Periodic Array of Arbitrary Volumetric Obstacles

Modeling High Frequency Propagation in Tunnel Environments by Iterative Physical Optics Method

The filter lowest-frequency transmission band arises from the effect of a Fabry-Perot interference filter at the resonance frequency of the temperature plateau.

The next (in frequency) transmission band appears at the cutoff frequency.

The higher-frequency transmission bands result from the antireflection of the atmosphere, an effect well-known in optics and acoustics.

Low frequency transmission of a plastid-encoded trait in Setaria italica

Electron transport properties of single crystal and polycrystalline natural mineral galena (PbS) samples from the Trep?a mine, Yugoslavia, were determined using the photoacoustic frequency transmission technique.

By investigating the cascade synthesis of lossless Single-end loaded network, this paper proposes the idea that synthesis can be realized for arbitrary real-frequency trasfer zeros by unrestrictedly using a ladder network without mutual inductance, and it also supplies a strict verification.Combining this method with the method which Lin Zaixu proposed in Document (1), the author gives a computer program for realizing transfer zeroes in all complex planes.

Based on the basic epuations of transmission lines,the relationship among the equivalent value,the working frequency and the connecting cable's length of capacitive transducer is drawn.And the effect of the last two on the relative sensitivity and linearity of the former is pointed out.Then,the principle of determining the woking frequency of capacitive trans- ducer and the length of its connecting cable is advanced.

Propagation of elastic waves along a borehole excited by acoustic multipole sources in soft formation was studied by using "real axis integration" and "branch cut integration". The full wave trains, the pure P and S waves and their excitation spactra have been given. Results obtained with the two numerical methods were compared with each other. It has been shown that: Pure P and S waves are undi-spersed and attenuated, and possess characteristic propagating frequencies respectively, except for the 5 wave under...

Propagation of elastic waves along a borehole excited by acoustic multipole sources in soft formation was studied by using "real axis integration" and "branch cut integration". The full wave trains, the pure P and S waves and their excitation spactra have been given. Results obtained with the two numerical methods were compared with each other. It has been shown that: Pure P and S waves are undi-spersed and attenuated, and possess characteristic propagating frequencies respectively, except for the 5 wave under the conditions of the P waves have a series of discrete characteristic frequencies, while the S waves have only one; the minimum of such frequencies of P waves is larger than that of S waves; when the pole number n increases, the two kinds of characteristic frequencies will become higher, and the difference between them will also become larger. Therefore, if the center frequency of acoustic sources is in the vicinity of S wave characteristic frequencies and far away from the P wave characteristic frequencies, the multipole sources with lower excitation frequencies can efficiently suppress P waves and excite strong S waves. The numerical results have also shown that the so called shear wave trains in general shear wave logs are composed of pure S waves and asymmetric modes at cut off frequencies, and their contributions to the full wave trains depond on the center frequencies of multipole sources and their frequency bands.