THE THEORY OF RADIO-WAVE PROPAGATION IN A NONHOMOGENEOUS ATMOSPHERE FOR A SLIGHTLY RAISED SOURCE

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Document Number (FOIA) /ESDN (CREST): 
CIA-RDP80-00809A000600350116-4
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RIPPUB
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C
Document Page Count: 
2
Document Creation Date: 
December 22, 2016
Document Release Date: 
August 19, 2011
Sequence Number: 
116
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Publication Date: 
October 3, 1950
Content Type: 
REPORT
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PDF icon CIA-RDP80-00809A000600350116-4.pdf102.95 KB
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Sanitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350116-4 1 CLASSIFICATION CONFIDEFiTIAI:~. :._1',eJ' CENTRAL INTELLIGENCE AGENCY REPORT INFORMATION FROM FOREIGN DOCUMENTS OR RADIO BROADCASTS CD NO. HOW PUBLISHED WHERE PUBLISHED DATE PUBLISHED LANGUAGE Bimonthly periodical Moscow Jan~Feb 1950 DATE OF INFORMATION ? 1950 DATE DIST. ~ Oct 1950 N0. OF PAGES 2 SUPPLEMENT TO REPORT N0. THIS IS UNEVALUATED INFORMAL-ION TNII DOCV Y[MT CONTAIN6 INIORYATION Af1[CTI Mf TN[ MATIONA[ D[I[NIl OS 'NL VNIT[0 iTAT[f MITNIM TMl RIAMIM6 01 [IIIOMAOI ACT f0 V. 6. C.. tl AND it. Af Ar[MDID. 1T1 TRANIrI3s10M OR TN[ RptLAT10x 01 I1f DOMT[NT! IN ANT?rAMN[N TO AM UNAVTNORII[0 IIRf ON IS IRO? NIRIT{D fT~AYI. R[IRODUCTION 0I 7X11 TORY If IROMI IIT[0. SOURCE Izvesti demii h ,Vol XN, No 1,.1950 PP 70-9 ? THE THEORY OF RADIO-WAVE PROPAGATION IN A NONHOMOGENEOUS ATMOSPHERE FOR A SLIGH7.'LY RAISED SOURCE Diges] The theory of radio-wave propagation in an atmosphere whose dielectric constant depends upon height has already been elaborated for the case where the sotu~ce is s vertical electric dipole placed?on the earth's .surface. On the other hand, the case of a raised source (horizontal and vertical, electri- cal and magnetic dipoles) has been considered under the assumption.of a homo- geneous atmosphere. This article gtudies the "combined" case: a raised dipole and nonhomogeneous atmosphere, The formulas derived in the first case above, for the general case where the index of rePractign behaves arbitrarily, were developed in great detail on the assumption of normal refraction, where radio-wave propagation possesses qualitatively the same nature as in a.homogeneous atmosphere. The case of auperredraction where the lower layer of the atmosphere acquires the character of a wave guide is of independent interest and deserves special consideration. This article discusses this case in detail. For its quantitative charalemroftic, it is ~Tery udeful to point out its si,'ni.larity to the nonatationary p quantum mechanics on the spreading of'weve packets in a given Pield of ?~rce; this similarity has remained unnoticed up to now. Tihe problem of radio-wave propagation under condit'_ans where the atmos- phere plays the role of a wave guifle was taken up also by P. Ye. Krasnustikin, who applied the method of.?normal Waves to plane-laminar and spherico-laminar media?(see his brochure,."!(etod Normal`nykh Voln v Primenenii k Problems Dal'nikh Radiosvyazey," 191+7, Moscow State. University). '?Krasnushkin's in- teresting research, however, has main7.y a qualitative character and leaves un- expL?ined aseries of essential mathematical. problems, par'bicularly the problems - 1 - 6~~~?9~a~~~,~'i~IRI CLASSIFICATION ,,, CONFIDENTIAL STATE ARMY !! f~, Sanitized Copy Appro~ve~d for Release 2011/09/14 :CIA-RDP80-00809A000600350116-4 Sanitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350116-4 CONFIDENTIAL of the sgectrum ("range") of complex eigenvalues of the "normal naves" end the problems. of the limiting conditions for the corresponding normal func- tions." Section 1 of the article describes the basic equations and limiting conditions of the problem. Section. 2 considers the approximate forms of the equations (Leonto- vlch's parabolic equation) with suitable limiting conditions and with the. conditions that determine the characteristic: ("singularity"). Section 3 draw the similarity between this problem as formulated and the nonstationary problem of quantum mechanics. Section 4 makes the transition to dimensionless quantities. Section 5 studies the properties of the partial solutions of the dif- ferential equations: Section:: 6 constructs from the previous differential equations the gen- eral solution in the form of a contour integral and in the form of a series. Section 7 then considers an example where the curve of the given index of refraction is assumed to be composed of two rectilinear portions. Section 8 gives the approximate formulas that ere similar to the semi- classical formulas of quantum mechanics for the determination of the coef - ficients of damping and the "altitude, factors." troblems encountered in the methodology or procedure of numerical calculations are not treated in the article. - 2 - ~a~~~~ ~~~ra~H~ia~ Sanitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350116-4