<?xml version="1.0" encoding="utf-8" ?>
<rss version="2.0">
<channel>
<title>Reports</title>
<copyright>Copyright (c) 2013 Utah State University All rights reserved.</copyright>
<link>http://digitalcommons.usu.edu/atmlidar_rep</link>
<description>Recent documents in Reports</description>
<language>en-us</language>
<lastBuildDate>Sun, 27 Jan 2013 01:54:47 PST</lastBuildDate>
<ttl>3600</ttl>








<item>
<title>The effects of model misspecification on linear regression coefficients as applicable to solar and linear terms</title>
<link>http://digitalcommons.usu.edu/atmlidar_rep/3</link>
<guid isPermaLink="true">http://digitalcommons.usu.edu/atmlidar_rep/3</guid>
<pubDate>Wed, 17 Aug 2011 09:34:04 PDT</pubDate>
<description>
	<![CDATA[
	<p>Determining atmospheric solar response from data is typically done by fitting a linear model to the data using a least squares approximation. These models typically include a solar proxy that follows the 11 year solar intensity variation, as well as a linear cooling trend. In this paper it is argued that such a regression model is flawed in that the atmospheric solar response might be out of phase with the solar input. And if so, the phase difference between solar input and atmospheric solar response can significantly bias the linear regression coefficient and attenuate the solar coefficient. This result is important because the sign of the solar response has been noted to change with altitude. Consequently, at some point between these two regions the solar response must go through zero, regardless of whether the actual solar response is zero at that altitude.</p>

	]]>
</description>

<author>Troy A. Wynn et al.</author>


</item>






<item>
<title>Temperature trends and episodic changes of the middle atmosphere over Logan Utah with consideration to model specification</title>
<link>http://digitalcommons.usu.edu/atmlidar_rep/2</link>
<guid isPermaLink="true">http://digitalcommons.usu.edu/atmlidar_rep/2</guid>
<pubDate>Wed, 17 Aug 2011 05:23:57 PDT</pubDate>
<description>
	<![CDATA[
	<p>A summary of the linear trends estimated from the USU Rayleigh Lidar (41.74o N, 118oW) temperature data set. The data set covers a time span from September, 1993 to August, 2003 and an altitude range of 45 to 80 km. The data set includes 584 data points at 45 km to 580 data points at 80 km. Cooling trend profiles are calculated and compared to results from other researchers. Collinearity and bias are also considered as issues that could affect the regression results. Also considered is the possibility that the Mt. Pinatubo eruption has influenced temperature trend estimates. This is important because the Pinatubo-related mesosphere temperature response occurred about the time the USU lidar came on line, which could be affecting our trend estimates. A visual comparison of the annual and semiannual oscillations are also presented.</p>

	]]>
</description>

<author>Troy A. Wynn et al.</author>


</item>






<item>
<title>Wind Climatology at 87 km above the Rocky Mountains at Bear Lake Observatory--Fabry-Perot Observations of OH</title>
<link>http://digitalcommons.usu.edu/atmlidar_rep/1</link>
<guid isPermaLink="true">http://digitalcommons.usu.edu/atmlidar_rep/1</guid>
<pubDate>Wed, 03 Aug 2011 15:42:23 PDT</pubDate>
<description>
	<![CDATA[
	<p>This paper presents the neutral -wind climatology at approximately 87-km 53 altitude from Utah State University's Bear Lake Observatory (BLO). a mid-latitude site 54 situated in the middle of the Rocky Mountains. The winds were determined using a very 55 sensitive Fabry-Perot interferometer (FPI) observing the OH Me inel (6-2) PI (3) line al 56 843 nm. The climatology. determined from monthly averages of the nightly evolution of 57 the geographic meridional and zonal wind components over forty· five months, has three 58 distinct seasonal patterns: winter (November- February), summer (May-Jul y), and late 59 Slimmer (August and September). The background zonal wind is eastward the whole year 60 except March and April. The background meridional wind is northward in winter and 61 southward during the rest of the year. In late summer. the winds exhibit a very strong 62 semidiurnal tidal variation almost every night. In summer, they exhibit a similar tidal 63 variation on enough nights that a semi diurnal pattern appears in the climatology. In 64 winter. the nighHo·night variability is so great that little structure is evident in the 65 climatology . These winds are compared to those from other techniques or sites: ~l 66 observations from UARS. FPI observations from Michigan, and MF radar observations. 67 While generally agreeing in relative amplitudes and i.n phase. differences do exist. 68 especially the weak semidiurnal tide at BLO in winter and a greatly reduced {tide at spring 69 equinox compared to late summer. It is likely that these differences arise from the 2 70 topographical generation of gravity waves by winds flowing over the Rocky Mountains. 71 The tidal variations are also compared to results from the global-scale wave model 72 (GSWM): our semidiurnal amplitudes arc considerably bigger except in winter, and our 73 phases vary from showing very good agreement in July, fair agreement in April and 74 January, and disagreement in October. These large differences may be evidence that 11011 - 75 linear effects are more important than realized. The behavior of the background winds is 76 consistent with different populations of gravity waves reaching 87 km in summer and 77 winter. The behavior of the semidiurnal tidal variation is consistent' with a strong 78 interaction between the tidal and gravity·wave wind fields, and is consistent with the 79 different summer and Winter gravity wave population s, and with a fall· spring asymmetry 80 characterized by much weaker gravity wave sources in late summer than near spring 81 equinox.</p>

	]]>
</description>

<author>V. B. Wickwar et al.</author>


</item>





</channel>
</rss>
