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A Semi-Implicit, Three-Dimensional Model for Estuarine ... - USGS

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120 A <strong>Semi</strong>-<strong>Implicit</strong>, <strong>Three</strong>-<strong>Dimensional</strong> <strong>Model</strong> <strong>for</strong> <strong>Estuarine</strong> Circulation<br />

Table 5.5. Definition of error measures (expressed as percentages) <strong>for</strong> the tidal test problem.<br />

[The first three error measures are based on comparisons between the computed solution and the base solution during the 11th tidal<br />

cycle at x =180,000 feet. The mass preservation error is computed as the maximum error (relative to the base solution) in total mass<br />

of water within the channel during each simulated time step]<br />

Description Definition<br />

Root mean square error: Root mean square error of<br />

the computed volumetric transport, normalized on the<br />

maximum volumetric transport of the base solution<br />

Amplitude error: Error in the maximum water<br />

surface elevation, normalized on the maximum water<br />

surface elevation of the base solution<br />

Phase error: Error in the time associated with the center<br />

of gravity of the computed water surface distribution,<br />

normalized on the time associated with the<br />

center of gravity of the base solution<br />

Mass preservation error: Maximum error in mass<br />

preservation <strong>for</strong> the computed solution, normalized<br />

on the total mass from the base solution<br />

t 1 = 7,440 minutes (= 124 hours)<br />

t 2<br />

n 1<br />

n 2<br />

= 8,190 minutes (= 136.5 hours)<br />

= t1 ⁄ Δt<br />

= t2 ⁄ Δt<br />

RMS e<br />

A e<br />

P e<br />

where<br />

nts11 = n2 – n1 nts = number of time steps in a 6 day simulation<br />

n<br />

Ub ( x)<br />

nts11<br />

∑<br />

100<br />

U n n<br />

( ( x)<br />

– Ub ( x)<br />

) 2<br />

n = n1<br />

( nts11)<br />

1 = ---------------------------------------------------------------------------<br />

⁄ max 2 Ub ( x)<br />

100 ζ max max<br />

( ( x)<br />

– ζb ( x)<br />

)<br />

= ---------------------------------------------------------max<br />

ζb ( x)<br />

100( Tx ( ) – Tb( x)<br />

)<br />

= --------------------------------------------<br />

Tb( x)<br />

Tx ( )<br />

M e<br />

t2 ∫t1 t2 ∫t1 x = 180,000<br />

1⁄ 2<br />

x = 180,000<br />

x = 180,000<br />

tHxt ( , ) H0 ζ min [ – ( + ( x)<br />

) ]dt<br />

Hxt ( , ) H0 ζ min = ----------------------------------------------------------------------------------<br />

[ – ( + ( x)<br />

) ]dt<br />

max E n<br />

= n = 1, 2 , ... , nts<br />

= volumetric transport <strong>for</strong> the base solution at location x and time t = nΔt<br />

Umax b ( x)<br />

= maximum volumetric transport <strong>for</strong> the base solution at location x (= 82.34 square feet per second at<br />

180,000 feet)<br />

max<br />

ζb ( x)<br />

= maximum water surface elevation <strong>for</strong> the base solution at location x (= 4.00 feet)<br />

ζ min ( x)<br />

= minimum water surface elevation at location x<br />

H0 = initial water depth in tidal channel (= 33.0 feet)<br />

L = length of channel (= 315,000 feet)<br />

Integrations were computed numerically with Simpson’s Rule.<br />

where<br />

E n<br />

=<br />

⎛ L<br />

⎞<br />

⎜ ∫0( Hxt ( , ) – ( H0 – 5)<br />

)dx⎟<br />

100⎜1– -------------------------------------------------------- ⎟<br />

L<br />

⎜ ⎟<br />

⎝ ( Hb( x, t)<br />

– ( H0 – 5)<br />

)dx⎠<br />

∫ 0<br />

t = nΔt

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