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We have made carefully calibrated radar scattering measurements by using the large 50‐MHz Jicamarca antenna. Typical results from the altitudes of maximum echo power for the vertically directed beam are σ radar ∼1–2 × 10 −10 m −1 for strong daytime electrojet conditions with type 1 irregularities present, with values a factor of 10 or so smaller during moderate conditions when only type 2 are observed. These cross sections, which are very large in comparison with those for incoherent scatter (σ radar ≃5 × 10 −18 m −1 for an electron density of 10 11 m −3 ), are not nearly large enough, however, to cause pseudo‐absorption events on riometer records, as was suggested by D'Angelo in 1976. If a model for the k dependence of the irregularities is assumed, it is possible to relate the radar data, which correspond to a single point in k ‐space, to in situ measurements of δn/n o , which correspond to a single point in physical space (an integral over the k ‐spectrum). The comparisons are reasonable, but depend significantly upon the assumed large scale cutoff for type 2 irregularities and the small scale cutoff for type 1.
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Farley et al. (1981) studied this question.
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