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Volume 1 - The Atmospheric Studies Group at TRC

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During execution, the bulk algorithm computes the sea-air differences from air<br />

measurements of wind speed, temper<strong>at</strong>ure, and humidity (w<strong>at</strong>er vapor), and w<strong>at</strong>er<br />

temper<strong>at</strong>ure, and iter<strong>at</strong>es to find the balanced set of scaling parameters u * , θ * , q * , and<br />

L th<strong>at</strong> s<strong>at</strong>isfy Equ<strong>at</strong>ion 3-12. Submodels for a cool-skin w<strong>at</strong>er surface temper<strong>at</strong>ure<br />

and for the diurnal warm-layer temper<strong>at</strong>ure structure in the upper few meters of the<br />

w<strong>at</strong>er column (Fairall et al., 1996) can be activ<strong>at</strong>ed to estim<strong>at</strong>e the w<strong>at</strong>er surface<br />

temper<strong>at</strong>ure from the temper<strong>at</strong>ure measured below the surface. <strong>The</strong> specific<br />

humidity <strong>at</strong> the w<strong>at</strong>er surface is obtained from the vapor pressure of sea w<strong>at</strong>er (0.98<br />

times th<strong>at</strong> of pure w<strong>at</strong>er) evalu<strong>at</strong>ed <strong>at</strong> the w<strong>at</strong>er surface temper<strong>at</strong>ure.<br />

An extension has been added in the CALMET implement<strong>at</strong>ion of the COARE<br />

algorithm to modify the roughness length z 0 (m) computed for shallow coastal areas.<br />

<strong>The</strong> COARE roughness length without wave model adjustments is given by:<br />

z<br />

0<br />

2<br />

0.11υ α u<br />

= +<br />

*<br />

(3-25)<br />

u g<br />

*<br />

where υ is the kinem<strong>at</strong>ic viscosity of dry air (~1.5x10 -5 m 2 /s), g is the acceler<strong>at</strong>ion<br />

due to gravity (m/s 2 ), and u * is the friction velocity (m/s). <strong>The</strong> Charnock parameter α<br />

is held <strong>at</strong> 0.011 for u 10 up to 10m/s and then it increases linearly to its maximum<br />

value of 0.018 <strong>at</strong> u 10 =18m/s. <strong>The</strong> first term is the aerodynamically smooth limit in<br />

which the thickness of viscous sublayer is inversely proportional to the wind stress.<br />

S<strong>at</strong>tler et al. (2002) describe a coupled ocean wave model (WAM) with the Danish<br />

Meteorological Institute High Resolution Limited Area Model (DMI-HIRLAM) for<br />

<strong>at</strong>mospheric forecasting. When the coupling to the wave model is turned off, the<br />

DMI-HIRLAM uses a larger Charnock parameter in shallow coastal w<strong>at</strong>ers. <strong>The</strong>y<br />

claim th<strong>at</strong> setting α = α c = 0.032 is supported by the measurements of Oost (1998),<br />

Hansen and Larsen (1997), and Ma<strong>at</strong> et al. (1991), although the wave age appears to<br />

be the parameter th<strong>at</strong> controls the increased roughness. <strong>The</strong>refore, a modifying factor<br />

for the Charnock parameter F α is introduced in CALMET. It multiplies the COARE<br />

Charnock parameter to cre<strong>at</strong>e a transition from a coastal value α c to the standard<br />

COARE value α over a length scale for the coastal region, L c :<br />

F<br />

α<br />

=<br />

1 −<br />

⎛<br />

⎜ 1 −<br />

⎝<br />

α<br />

c<br />

α<br />

⎞<br />

⎟<br />

⎠<br />

exp<br />

⎡<br />

⎢ −<br />

⎢⎣<br />

⎛<br />

⎜<br />

⎝<br />

x<br />

L<br />

c<br />

⎞<br />

⎟<br />

⎠<br />

4<br />

⎤<br />

⎥<br />

⎥⎦<br />

(3-26)<br />

This factor is order α c /α for distances less than 0.5L c , and is order 1 for distances<br />

gre<strong>at</strong>er than 1.5L c .<br />

Two wave parameteriz<strong>at</strong>ions are also available in the COARE module:<br />

• wave=1: use the Oost et al. (2002) wave-age parameteriz<strong>at</strong>ion<br />

Final Report Vol.1 11

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