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64<br />
3. Results<br />
Fig. 2 shows the analysis of sensitivity of summer (JJA)<br />
time-averaged precipitation to a moderate perturbation of the<br />
threshold vertical velocity in the trigger function of the<br />
Kain-Fritch deep convection scheme. This parameter is<br />
perturbed from its standard value of 3.4 cm/s to 4.8 cm/s. In<br />
Fig. 2 the noise standard deviation (a), the signal (b) and the<br />
level of rejection of H 0 (c), all computed for summer<br />
precipitation are shown. Results obtained with the large<br />
domain are on the left and those with the small domain on<br />
the right.<br />
It can be seen that internal variability noise standard<br />
deviation in the large domain (Fig. 2a, left) exhibit very<br />
large values that locally reach 2 mm/day. In the same time,<br />
in response to the parameter perturbation (Fig. 2b, left),<br />
there is a decrease of precipitation over the continent and the<br />
southeast portion of the domain, comparable to the noise<br />
level. The signal is scarcely distinguishable from internal<br />
variability since the level of rejection of H 0 is predominantly<br />
below 90% (Fig. 2c, left).<br />
Clearly, more simulations with perturbed initial conditions<br />
are necessary to provide statistical significance in the large<br />
domain. Some more confidence can be attributed to the<br />
signal pattern over the continent, since a perturbation of<br />
the same parameter and magnitude but of the opposite sign<br />
produces a similar pattern of model response but with the<br />
opposite sign (not shown). This indicates a strong linear<br />
component of the sensitivity to the given parameter. It is<br />
also worth noting that the internal variability exhibits a<br />
pronounced annual cycle, with maximum in summer and<br />
minimum in winter. Hence, the rejection level of H 0 is<br />
larger in the remaining seasons. However, the magnitude<br />
and the pattern of the signal also considerably vary<br />
through seasons.<br />
Reduction of domain size decreases the noise<br />
magnitude roughly by factor of 3 (Fig. 2a, right). In the<br />
same time, comparison of Figs. 2b left and right shows no<br />
evidence that the sensitivity of summer precipitation is<br />
reduced. One exception is the area of the positive<br />
sensitivity off the coast of Virginia. Over land the absolute<br />
change in precipitation is locally even larger in the smaller<br />
domain. This is reflected in a substantial increase in<br />
statistical significance of the signal: the level of rejection<br />
of H 0 becomes larger than 99% over a considerable part of<br />
the area of comparison (Fig. 2c, right).<br />
4. Discussion and concluding remarks<br />
It is clear that reduction in domain size decreases the<br />
computational cost of the PPE, both directly through<br />
reduction of the number of computational points and<br />
indirectly – reducing the number of identical simulations<br />
with perturbed initial conditions needed to provide the<br />
statistical significance of the signal. Given that the<br />
computational resources are usually limited by external<br />
funding and thus non-negotiable, the lowering of noise is<br />
an important advantage of the small domain because it<br />
allows allocation of resources to the PPE size (e.g., more<br />
parameters and perturbations can be included in the<br />
study). Furthermore, noise can render very difficult the<br />
quantification of non-linear components of the model<br />
response to simultaneous multiple-parameter<br />
perturbations.<br />
There are, however, two important disadvantages of the<br />
small domain to be noted. Firstly, the results obtained in<br />
the small domain are representative for a small region and<br />
are of little value for typical RCM domains to which this<br />
study is addressed. Secondly, it can be argued that in a too<br />
small domain, control of the large-scale interior flow by<br />
the LBC may be excessive and suppress the signal.<br />
Suppression of the model sensitivity to parameter<br />
perturbations would decrease spread among the members<br />
of the PPE and yield an underestimation of the uncertainty<br />
range with respect to that in typical RCM simulations. Our<br />
results provide no evidence that this happens with seasonal<br />
precipitation but the concern still remains when less smallscale<br />
dominated variables are considered.<br />
References<br />
Figure 2. Summer seasonal-average precipitation<br />
(left – large domain, right – small domain): (a)<br />
internal variability noise standard deviation (mm/day);<br />
(b) change in response to positive perturbation of the<br />
threshold vertical velocity in the Kain-Fritch deep<br />
convection (mm/day), and (c) the statistical<br />
significance of the change (%).<br />
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Quantification of the Lateral Boundary Forcing of a<br />
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