Search Results

You are looking at 1 - 10 of 27 items for

  • Author or Editor: Thomas McKee x
  • Refine by Access: All Content x
Clear All Modify Search
Thomas B. McKee

Abstract

No Abstract.

Full access
Thomas McKee and Stephen K. Cox

Abstract

Calculated distributions of scattered shortwave radiance are presented for simulated cumulus clouds using a cubic shape. Comparison with similar clouds of semi-infinite horizontal extent is included. For an incident solar zenith angle of 0° the angular distribution of the radiance exiting the cloud top is similar for the cube and the semi-infinite layer, but the radiance from the cube is much smaller for optical depths between 9.8 and 73.5. At an optical depth of 73.5 the vertical radiance from the cube is only 58% of the radiance from the semi-infinite layer cloud. For an incident solar zenith angle of 60°, the angular distribution and the magnitudes of the scattered radiances are similar for the cube top and the semi-infinite layer. A comparison of the total radiance from the cube top and side in the solar plane shows a dramatic change in angular distribution compared with the semi-infinite cloud. Radiances exiting the antisolar side of the cube illustrate the strong forward scattering for short optical paths near cloud edges. The transition from cubic clouds to semi-infinite layers is illustrated for a vertical sun. Results indicate a rapid change for width-to-depth ratios of 1–4 followed by a slower asymptotic change.

Full access
Georg J. Mayr and Thomas B. McKee

Abstract

The evolution of low-level flow upstream of the Continental Divide (Rocky Mountains) and the Wasatch Range from being unable to surmount the mountain range, to becoming unblocked and blocked again is studied observationally. During two months in the winter of 1991/92, a transect of three wind profilers measured the wind field every few minutes with unprecedented temporal detail.

The average state of that region during winter is blocked. A total of 47 blocked events were observed. A blocked flow event lasted on the average one and a half days, but the duration varied widely from a few hours to eight days controlled by the synoptic situation. The transition between the two states happened rapidly on the order of 1 h with a minimum of 20 min and a maximum of 4 h. The depth of the blocked layer during one blocking episode fluctuated considerably but reached on the average one-half to two-thirds of the barrier depth (depending on the location).

Previous research of idealized equilibrium situations focused on changes of the cross-barrier wind speed and stability as determining variables to build a mesoscale high over the barrier. Since their values were in the blocked range, other mechanisms had to trigger the transitions to an unblocked state.

A conceptual model proposes synoptic and radiative forcing to drive the blocking evolution. When the mountain-induced mesoscale high blocks the low-level flow, an opposing synoptic cross-barrier pressure gradient can negate the mesoscale high. Therefore unblocking happens most frequently when the trough axis of a short wave is immediately upstream of the harder, but synoptic pressure gradients caused by contrasts in vorticity and differential temperature advection are sometimes also strong enough. The flow returns to its blocked state when the ridge behind the trough approaches the barrier so that the synoptic cross-barrier pressure gradient reinforces the mesoscale high.

For a lower barrier or stronger solar insulation, a well-mixed boundary layer can grow almost to the height of the barrier by afternoon and reconnect the blocked layer with the higher cross-barrier winds above the mountain. After sunset the thermal forcing changes sign as the radiative cooling stabilizes the lower atmosphere again and the transition back to the blocked state occurs.

Full access
C. David Whiteman and Thomas B. McKee

Abstract

A thermodynamic model is developed to simulate the evolution of vertical temperature structure during the breakup of nocturnal temperature inversions in mountain valleys. The primary inputs to the model are the valley floor width, sidewall inclination angles, characteristics of the valley inversion at sunrise, and an estimate of sensible heat flux obtained from solar radiation calculations. The outputs, obtained by a numerical integration of the model equations, are the time-dependent height of a convective boundary layer that grows upward from the valley floor after sunrise, the height of the inversion top, and vertical potential temperature profiles of the valley atmosphere. The model can simulate the three patterns of temperature structure evolution observed in deep valleys of western Colorado. The well-known inversion breakup over flat terrain is a special case of the model, for which valley floor width becomes infinite. The characteristics of the model equations are investigated for several limiting conditions using the topography of a reference valley and typical inversion and solar radiation characteristics. The model is applied to simulate observations of inversion breakup taken in Colorado's Eagle and Yampa Valleys in different seasons. Simulations are obtained by fitting two constants in the model, relating to the surface energy budget and energy partitioning, to the data. The model accurately simulates the evolution of vertical potential temperature profiles and predicts the time of inversion destruction.

Full access
Nolan J. Doesken and Thomas B. McKee

Abstract

A methodology has been developed to estimate winter design temperatures (temperatures exceeded a specific number of hours during the December through February winter season-an important design parameter in building construction) from synthetic distributions of hourly temperatures for locations where only daily maximum and minimum temperatures are observed. Cumulative distributions of hourly temperatures and daily minimum temperatures were examined at seven different locations in Colorado having 10 or more consecutive years of complete hourly data. A consistent relationship between the two distributions was found for these stations by representing the lower half of each distribution with a best-fit power curve and relating the fitting coefficients. From these relationships an equation was derived that generated the shape of the lower half of the cumulative distribution of hourly temperatures. The only required input parameters are the regression coefficients resulting from the power curve fitting of the observed distribution of daily minimum temperatures.

The method was tested in Colorado stations having both hourly and daily temperature data. Excellent results were obtained for Colorado. Synthesized temperatures at probabilities of up to 0.50 were generally within 0.7°C of the observed values. The method has now been employed to calculate winter design temperatures for dozens of Colorado cities where such information has previously been unavailable.

Full access
David M. Ebel and Thomas B. McKee

Abstract

One of the important radiative effects of cloud Shape is to modify diurnal radiance patterns observed from satellites. Theory predicts a diurnal radiance pattern nearly symmetric about local noon for both semi-infinite and finite clouds situated on the equator at the equinox with a satellite directly overhead. For a geostationary satellite (SMS-1) located to the west of the cloud, the semi-infinite cloud still products a pattern nearly symmetric about local noon while finite cubic clouds produce a distinctly different pattern which peaks during the afternoon. Simulated diurnal satellite observations of a finite cubic and semi-infinite cloud were compared with actual diurnal satellite observations of cloud fields with cloud cover varying from less than 30% to greater than 90%. The results for 4 n mi resolution data from the two observed cloud fields demonstrate that the diurnal radiance patterns of both semi-infinite and finite clouds exist in satellite observations. Degrading the resolution to 16 n mi did not significantly alter the semi-infinite or finite diurnal radiance pattern of either observed cloud field. The effects of cloud shape on satellite observations have potential application to problems in data interpretation, cloud cover determination, albedo calculations and identification of cloud fields.

Full access
David C. Bader and Thomas B. McKee

Abstract

A dry two-dimensional version of the Colorado State Cloud/Mesoscale Model was used to study the morning, inversion destruction cycle in a variety of deep mountain valley configurations. Eleven simulations were run to examine the effects of valley width, surface heating rate, wind shear above the valley, valley orientation, sidewall slope, initial stability and variable surface albedo on the evolution of the daytime boundary layer in the valley. Each was initiated with a stable layer filling the valley to ridgetop with a neutral layer above the ridge. The model was driven at the lower surface by a sinusoidally varying potential temperature flux which approximates the diurnal heating cycle. All simulations show that the initial inversion layer is destroyed by a combination of three processes; a growing surface based neutral layer over the valley floor, the destabilization of the stable air mass by the recirculation of air warmed over the slopes and the descent of the inversion top by the transport of air beneath the stable layer out of the valley in the slope flows.

The results show a wide variety of boundary layer behavior typical of that observed in several western Colorado valleys. Most of the model inversions were destroyed 3.5–5 h after sunrise, which is consistent with thermodynamic calculations. Slope effects decrease with increasing valley width and become unimportant when ridgetop width-to-depth ratios exceed 24. Decreasing the surface heating rate influences the rate but not the structure of the boundary layer development. A very weakly heated valley, typical of those with a high surface albedo due to snow, will hold a stable layer until very late in the day. Moderate wind shear and valley orientation have very little effect on the simulated boundary layer evolution. Steeper sidewall slopes and stronger initial stabilities inhibit slope flow development and exhibit less inversion descent. Conversely, lower surface albedos along the valley sidewalls can dramatically increase the magnitude of the stable layer descent.

Full access
Thomas B. McKee and John T. Klehr

Abstract

Calculations are presented which compare the effects on directional reflectance and relative radiance of changes in microphysical structure and geometric shape for scattered solar radiation in terrestrial water clouds. The effect of changes in microphysical structure was relatively small and was 5.5% in directional reflectance for cloud optical depth of 60 and solar zenith of 23.0°. In contrast, effects of changes in geometric shape from a semi-infinite layer to a cube of optical depth 60 were 35%. Narrow turrets growing above a base cloud are shown to be darker than the base cloud with a reduction in relative radiance of 34.5% for a vertical sun. Directional reflectances for turret clouds are smaller than for clouds with flat tops due to the presence of additional edges. It appears that the interactions between the turret and the base cloud represent a small effect compared to the addition of more edges and surface area of the turret. Cumulus clouds in nature contain many more surface features which, although less sharp than in this model, undoubtedly contribute to a reduced directional reflectance.

Full access
Paul G. Wolyn and Thomas B. McKee

Abstract

A deep stable layer (DSL) is a layer much deeper than a typical nocturnal inversion with stabilities not frequently found over a sizable portion of the lowest 1.5 km. They have traits that can cause the stagnation of cold air in basins, i.e., light winds at the surface even if moderately strong winds aloft are present, and the restriction of the growth of daytime convective boundary layers. The objective definition used in this study is that, if 65% of the lowest 1.5 km of the 1200 UTC [0500 mountain standard time (MST)] sounding has a lapse rate of 2.5°C km−1 or less, then the day is under the influence of a DSL. A climatology of days under the influence of a DSL was performed at four sites in the intermountain western United States: Grand Junction, Colorado; Salt Lake City, Utah; Winnemucca, Nevada; and Boise, Idaho. The DSL is a wintertime phenomenon with 10% to 20% of the days in December and January at the four stations being under the influence of a DSL. Successive days with a DSL present lead to episodes of varying lengths. Episodes of three days or longer occurred at least once each year at Boise and Grand Junction and at least once every two years at Salt Lake City and Winnemucca. An episode of 8 days duration occurred at Grand Junction.

A DSL episode that occurred in December 1980 was examined in depth to gain insight into the life cycle of a DSL. Synoptic-scale warming above 1 to 1.5 km and weak surface heating were important for the initiation of the episode. The longwave radiation properties of a persistent fog layer and weak surface heating were important physical processes for maintaining and prolonging the episode. From the episode it is hypothesized that DSLs form when warming aloft traps relatively cold air near the surface, decoupling it from the rest of the atmosphere. The barriers surrounding the basins are important for the formation of a DSL because they prevent the horizontal movement of the cold air. DSLs have important implications for air quality, episodes of persistent fog, and surface temperature forecasts.

Full access
Paul G. Wolyn and Thomas B. Mckee

Abstract

The daytime mountain-plains circulation east of a 2-km-high and 60-km-wide barrier is examined for conditions of clear skies, light ambient winds with a westerly component around 5 m s−1, and little spatial and temporal change to the synoptic-scale thermal fields and wind fields. Fourteen nonhydrostatic, two-dimensional, horizontally homogeneously initialized simulations, employing the Colorado State University Regional Atmospheric Modeling System, are used to study the important physical processes in the daytime evolution. A synthesis of simulations with various initial conditions and boundary conditions are used to derive a conceptual model of the daytime evolution. The simulations am run for different times of the year, different patterns of soil moisture (which affects the surface sensible heat flux), different ambient winds, different thermal structures, half-barrier height, and absence of a nighttime phase. Except for the simulation without a nighttime phase, the simulations have a full nighttime phase before the daytime evolution is studied. Observations, consisting of frequent (every 2–3 h) airsonde launches from sunrise until the afternoon in the vicinity of Fort Collins, Colorado, are used to gauge how well the simulations match the daytime evolution. The simulations and observations qualitatively agree well, showing that the simulations satisfactorily re-create the daytime evolution.

The variety of simulations and observations show a complex sunrise state that is not close to horizontally homogeneous. The sunrise state has a complex interaction between the thermally driven nocturnal flows and the ambient flow. Three distinct phases appear in the daytime evolution. Phase 1 results from the weakening nocturnal flows interacting with the daytime heating, and it lasts until 3–4 h after sunrise. Phase 2 is characterized by a developing solenoid. The solenoid is not horizontally or vertically symmetric, and it has two stages of development. Phase 2 lasts until at least 7 h after sunrise, and it can exist until sunset. The main feature in phase 3 is a migrating solenoid moving beneath the leading edge of the cold core. This phase exists from the end of phase 2 until near sunset, and this phase does not exist on all days. The migrating solenoid is a disturbance (which can significantly influence the atmosphere east of the barter) in the main daytime circulation.

The simulations generally show that for phases 2 and 3 the circulation is weaker and shallower for moister soil on the eastern plains (less surface sensible heat flux), moister soil west of the barrier crest, days closer to the winter solstice, stronger ambient winds, and lower convective boundary layer (CBL) the previous day. The circulation is generally deeper and stronger for less stability (after 5 h after sunrise) and for times closer to the solstice, especially by 5 h after sunrise. The CBL on the eastern plains is shallower for moister soil on the eastern plains, days closer to the winter solstice, stronger ambient winds, and lower CBL the previous day (after the solenoid passes). The proper boundary and initial conditions are needed to accurately simulate the daytime evolution. Inclusion of the nighttime phase is important to properly replicate the daytime evolution, especially the sunrise state and phase 1. The evolution east of a 1-km-high barrier is different from an evolution east of a 2-km-high barrier. In a simulation without ambient winds, the sunrise state is significantly different from the simulations with ambient westerly flow with phases 1 and 3 being absent.

Full access