1990
DOI: 10.1029/rs025i004p00289
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Signal frequency dependence of ionospheric amplitude scintillations

Abstract: The S4 index, which is a measure of the strength of amplitude scintillations, is assumed to vary with signal frequency f according to S4 ∝ f−n, and the frequency exponent n is derived from observed equatorial amplitude scintillations on 40‐ and 140‐MHz signals. A large data base has been used to study the variation of this exponent n(40/140) with the S4 index on the 140‐MHz signal for both daytime and nighttime scintillation events. Although the equatorial E and F region irregularities, which cause the observe… Show more

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Cited by 8 publications
(9 citation statements)
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“…Scintillations were also recorded on a L1 (1.575 GHz) signal transmitted from the geostationary satellite GSAT-10 (PRN 128) located at 83°E and received at MUM and at the equatorial station Trivandrum (TRV) located close to TIR. For weak scintillations produced by EPB irregularities, which are highly elongated in the direction of the geomagnetic field and hence may be considered to be essentially two dimensional, with a power law irregularity spectrum of the form Φ ΔN (q) ∝ q À m , the S 4 index is expected to show a signal frequency (f) dependence of the form: S 4 ∝ f À n , where n = (m + 3)/4 [Yeh and Liu, 1982;Bhattacharyya et al, 1990]. However, in the present case, S 4 on the 251 MHz signal exceeds 1, where the signal frequency dependence of S 4 departs significantly from the weak scintillation case.…”
Section: Latitudinal Variation Of Vhf and L-band Amplitude Scintillatmentioning
confidence: 99%
“…Scintillations were also recorded on a L1 (1.575 GHz) signal transmitted from the geostationary satellite GSAT-10 (PRN 128) located at 83°E and received at MUM and at the equatorial station Trivandrum (TRV) located close to TIR. For weak scintillations produced by EPB irregularities, which are highly elongated in the direction of the geomagnetic field and hence may be considered to be essentially two dimensional, with a power law irregularity spectrum of the form Φ ΔN (q) ∝ q À m , the S 4 index is expected to show a signal frequency (f) dependence of the form: S 4 ∝ f À n , where n = (m + 3)/4 [Yeh and Liu, 1982;Bhattacharyya et al, 1990]. However, in the present case, S 4 on the 251 MHz signal exceeds 1, where the signal frequency dependence of S 4 departs significantly from the weak scintillation case.…”
Section: Latitudinal Variation Of Vhf and L-band Amplitude Scintillatmentioning
confidence: 99%
“…Over the past two decades, many excellent reviews of scintillation theory and observations have been published (e.g., Aarons, 1982Aarons, , 1993Yeh and Liu, 1982;Basu, 1985, 1993;Rastogi, 1985, 1991;Bhattacharyya et al, 1990Bhattacharyya et al, , 1992. Comprehensive reviews of the physics of ionospheric irregularities can also be found in many articles (e.g., Keskinen and Ossakow, 1983;Heppner et al, 1993;Fejer, 1996).…”
Section: Introductionmentioning
confidence: 99%
“…According to Bhattacharyya et al [1990], the frequency exponent (n) for weak scintillation is related to the power law index (m) for a two‐dimensional irregularity power spectrum through: therefore m can be estimated from n using the following equation: For the three examples in this paper, the power law indices of the intensity (m) are calculated and are equal to 5.88, 4.40, and 5.56, respectively.…”
Section: Sample Resultsmentioning
confidence: 99%
“…[14] According to Bhattacharyya et al [1990], the frequency exponent (n) for weak scintillation is related to the power law index (m) for a two-dimensional irregularity power spectrum through: n ¼ m þ 3 ð Þ =4; for 1 < m < 5; therefore m can be estimated from n using the following equation:…”
Section: Example 3: Prn06 (Svn03) Quiet Day (6 December 1989)mentioning
confidence: 99%