1973
DOI: 10.1086/151987
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Direct Measurements of Solar-Wind Fluctuations Between 0.0048 and 13.3 HZ

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Cited by 65 publications
(37 citation statements)
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“…The values of the slopes and the frequencies of point intersections of these lines (breakpoint 1 and breakpoint 2 in the figure) are shown in figure 2b, together with the slope of the Kolmogorov spectrum −5/3 (dashed line). A similar spectrum with flattening around ion scales was first observed in [13,14,16,17,42]. Safrnakova et al [37] have shown that the breakpoint locations are controlled by the gyro-frequency.…”
Section: Introductionsupporting
confidence: 69%
See 1 more Smart Citation
“…The values of the slopes and the frequencies of point intersections of these lines (breakpoint 1 and breakpoint 2 in the figure) are shown in figure 2b, together with the slope of the Kolmogorov spectrum −5/3 (dashed line). A similar spectrum with flattening around ion scales was first observed in [13,14,16,17,42]. Safrnakova et al [37] have shown that the breakpoint locations are controlled by the gyro-frequency.…”
Section: Introductionsupporting
confidence: 69%
“…We discuss these results in §3. High-resolution plasma data were earlier accomplished up to 13.3 Hz by SW flux measurements in the OGO-5 experiment [17], up to approximately 5 Hz by electron density measurements in ISEE-1 and ISEE-2 experiments [13,14] and up to 2.5 Hz by electron density measurements on the CLUSTER experiment [16]. However, these authors did not note the steepening of the spectra.…”
Section: Introductionmentioning
confidence: 99%
“…In Figure 1 some synthetic density data calculated from published density power spectra are shown [Unti et al, 1973;Neugebauer, 1975Neugebauer, , 1976Celniker et al, 1983Celniker et al, , 1987. To make these curves, which essentially means reconstructing a time series statistically similar to the original data from which the power spectra were calculated, we have calculated a Fourier series for a much longer time period than shown (100 times longer), in which each amplitude is proportional to the square root of the power spectrum, integrated over the increment in frequency appropriate to a harmonic coefficient of the longer time period, and we have given the Fourier amplitude a random phase between 0 and 2•z and then done an inverse transform.…”
Section: Density Fluctuations the Wkb Approximation And Mode Evolutionmentioning
confidence: 99%
“…It is possible that the irregularity spectrum extends below '" 6 km (i.e. beyond 10 Hz) since all observed IPS spectra (and the spectra of Unti et al 1973) show no signs of tapering off at high frequencies. The spectra all meet the noise before any such effect is observed.…”
Section: Discussionmentioning
confidence: 99%