(3) The ∑Ce/∑Y proper values of the all kinds of the soils derived from different parent materials were 3.5-4.7. The characteristic of the fractional distillation between ∑Ce and ∑Y was obvious.

The Ti:LiNbO_3 waveguide switches can become tunable wavelength division mul- tiplexers and demultiplexers by choosing proper values of their configration and applied vol- tages of the switches.

In order to study the tempereture stresses of supporting structures, the openings between contact surfaces and the anchoring stresses under different free anchor bar lengths, by means of 3D FEM calculation for simulating the tempereture creep stresses in the construction period and nonlinear analyses to the adjacent contact problems between concrete structures and rock mass, the problems for taking proper values of the free lengths of anchor bar may be resolved.

In residual-stress measurement by the holedrilling technique, accuracy can be enhanced if the proper values for the relleved-strain coefficients are employed.

Secondly, a unique circuit structure is determined by selecting the proper values for the parameters that characterize the floating-gate inverters.

A number of bounded and linearly constrained parametric models are tested and convergence to proper values occurs from a wide range of initial error, utilizing minimal matching information (relative to the number of parameters and components).

We study the mean quadratic error of an estimate of splines of the first order, which is obtained by the method of least squares under the assumption that the data represents a superposition of proper values of a spline and a white noise.

We study the mean quadratic error of an estimate of splines of the first order, which is obtained by the method of least squares under the assumption that the data represents a superposition of proper values of a spline and a white noise.

Abstract—We have calculated the binding energies of atomic nuclei by using the theory of density matrices. Treating the binding energies of atomic nuclei as functionals of density matrices and applying the variational principle, we obtain the proper values of nuclear binding energies and nuclear radii. If the nucleonic interaction potential is taken as a Gaussian well of purely central fore with its interaction constants determined by low energy experiments and its exchange interaction double the ordinary...

Abstract—We have calculated the binding energies of atomic nuclei by using the theory of density matrices. Treating the binding energies of atomic nuclei as functionals of density matrices and applying the variational principle, we obtain the proper values of nuclear binding energies and nuclear radii. If the nucleonic interaction potential is taken as a Gaussian well of purely central fore with its interaction constants determined by low energy experiments and its exchange interaction double the ordinary interaction, it is able to obtain theoretical results in resonable agreement with the empirical data. The nuclear radii are 1.2×10~(-13) A~(1/3) cm, and the nuclear binding energies are even-even nuclei,odd mass nuclei, odd-odd nuclei.

The paper shows a way to utilize the property of convergence iu boundary condition that is characterized by the transfer matrices method in the whole process for calculating any certain modality of torsionl system with multidegrees of freedom. The proper values and the proper vectors may be gained from iteration simultaneously by repeatedly using the Holzer's table with a known region of a proper value. It is further simplified with a more rapid convergence rate and a higher iterating precision....

The paper shows a way to utilize the property of convergence iu boundary condition that is characterized by the transfer matrices method in the whole process for calculating any certain modality of torsionl system with multidegrees of freedom. The proper values and the proper vectors may be gained from iteration simultaneously by repeatedly using the Holzer's table with a known region of a proper value. It is further simplified with a more rapid convergence rate and a higher iterating precision.

This paper is a part of the result of the research on the electromagnetic analysis of the large-current isolated-phase enclosed bus. On the basis of the previous paper [5], the first part, which is about the a-c steady state, deals with the calculations of the enclosure currents of the 3-phase continuous type of bus, of the enclosure loss of tne discontinuous as well as the continuous type, and of the magnetic field outside the enclosures. The second part is about the transient state during short-circuits. On...

This paper is a part of the result of the research on the electromagnetic analysis of the large-current isolated-phase enclosed bus. On the basis of the previous paper [5], the first part, which is about the a-c steady state, deals with the calculations of the enclosure currents of the 3-phase continuous type of bus, of the enclosure loss of tne discontinuous as well as the continuous type, and of the magnetic field outside the enclosures. The second part is about the transient state during short-circuits. On the basis of another paper by the author [2], this part deals with the calculations of the enclosure currents of the 3-phase continuous type due to the d-c component of the short-circuit currents, of the magnetic field strength of other phases that penetrates into the enclosure, and finally, of the electro-magnetic force upon tne bus conductor caused by this field. The results of calculations applying all these methods have been checked by tests.All the formulas developed are general ones, and the calculations may be performed on computers. By inserting proper values of the parameters, the items mentioned above can be calculated for different cases including those of the continous enclosure with reactors and of 1-phase system.