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Fourth Study Conference on BALTEX Scala Cinema Gudhjem

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Statistic Parameters<br />

Qср, m 3 /sec σ, m 3 Period of<br />

average<br />

estimati<strong>on</strong><br />

/sec r(1)<br />

max min max min max min<br />

20 years 231 118 49,7 24,1 0,50 -0,43<br />

30 years 219 181 47,5 24,4 0,52 -0,27<br />

35 years 216 183 46,2 26,6 0,46 -0,24<br />

50 years 209 187 44,2 30,3 0,42 -0,12<br />

Table 2. Statistic parameters of moving average estimati<strong>on</strong><br />

of the Neman’s water flow at Grodno.<br />

As shown in Table 2, the maximum and minimum values<br />

pertaining to different periods of average estimati<strong>on</strong> vary<br />

greatly. This is caused by the period of the 1920s to the<br />

1940s with relatively high water levels in the Neman. Such<br />

differences in the parameter estimati<strong>on</strong> underline the instability<br />

hypothesis in respect of the time period in questi<strong>on</strong>.<br />

The verificati<strong>on</strong> of the hypothesis of statistic parameter homogeneity<br />

supports the above hypothesis.<br />

At present, 3 statistic models are generally used for the purpose<br />

of describing l<strong>on</strong>g-term flow fluctuati<strong>on</strong>: the sequence<br />

of independent c<strong>on</strong>tingency values, the simple Markov<br />

chain, and the complex Markov chain. The applicati<strong>on</strong> of<br />

the statistic c<strong>on</strong>cepti<strong>on</strong> is based <strong>on</strong> the principles of stability<br />

of the process and annual completeness of the observed data<br />

(Ismailov G.H, Fedorov V.M., 2001).<br />

If no trend is clearly detectable, it is necessary that selected<br />

Self-Correlati<strong>on</strong> (SCF) and Particular Self-Correlati<strong>on</strong><br />

(PSCF) Functi<strong>on</strong>s be c<strong>on</strong>sidered. These functi<strong>on</strong>s specify<br />

the type and the order of the annual river flow. SCF and<br />

PSCF of the Neman river at Grodno have a c<strong>on</strong>spicuous<br />

variati<strong>on</strong> with τ=1, while all other ordinate values prove to<br />

be statistically insignificant and are characterized by the alternati<strong>on</strong><br />

of positive and negative values. It follows that the<br />

process of the annual flow may be identified with the following<br />

model (Ismailov G.H, Fedorov V.M., 2001; Box<br />

G.E.P., Jenkins F.M, 1974):<br />

Q( t ) = Qср<br />

+ r(<br />

1 ) ⋅[<br />

Q(<br />

t −1)<br />

− Qср<br />

] + ξ(<br />

t ) , (1)<br />

where ξ ( t ) is the Gaussian “white noise”<br />

2<br />

and σξ = σQ<br />

⋅ 1 − r(<br />

1)<br />

.<br />

According to equati<strong>on</strong> (1), the annual flow of water in the<br />

Neman at Grodno is described with r(1)=0,19, Qср=194 m 3 /sec (Table 1), σξ = 36,19 m 3 /sec and σ Q =36,86<br />

m 3 /sec, resulting in<br />

Q( t ) = 0 , 19⋅<br />

Q(<br />

t −1)<br />

+ 157 + ξ(<br />

t ) .<br />

In this case the variance of the c<strong>on</strong>tingent c<strong>on</strong>stituent is<br />

quite high.<br />

The results c<strong>on</strong>cerning the l<strong>on</strong>g-term fluctuati<strong>on</strong>s of the annual<br />

flow of water in the Neman river at Grodno indicates<br />

the possible existence of a certain interc<strong>on</strong>necti<strong>on</strong> between<br />

c<strong>on</strong>secutive flow events. For this reas<strong>on</strong> the Markov simple<br />

chain can be applied to describe the annual flow of water,<br />

i.e.<br />

Q( t ) = r(<br />

1 ) ⋅Q(<br />

t −1)<br />

+ ξ(<br />

t ) . (2)<br />

The first item in the right part of equati<strong>on</strong> (2) may be interpreted<br />

as the river flow part caused by accumulated atmospheric<br />

precipitati<strong>on</strong> in the river basin during the previous<br />

year and its discharge into the river this year. In this case the<br />

c<strong>on</strong>tingent c<strong>on</strong>stituent ξ ( t ) in (2) must obviously include<br />

- 142 -<br />

that part of the annual outflow of the current year. The result<br />

(2) may be transformed into the following equati<strong>on</strong>s:<br />

Q( t ) = 0, 059⋅<br />

Q(<br />

t −1)<br />

+ 0,<br />

493⋅Woc(<br />

t ) + 71,<br />

02 + ξ(<br />

r1<br />

)<br />

(3)<br />

Q( t ) = 0, 205⋅Woc(<br />

t ) + 0,<br />

120⋅Woc(<br />

t −1)<br />

− 9.<br />

173 + ξ(<br />

t2<br />

)<br />

(4)<br />

where Woc( t ) and Woc( t − 1)<br />

denote the annual precipitati<strong>on</strong><br />

of the current and the previous years, respectively.<br />

The coefficient of multiple correlati<strong>on</strong> between the outflow<br />

and the defining factors in the equati<strong>on</strong> (3) is R=0,48>R Т (45, 5<br />

%)=0,29, while the ±5% and ±10% c<strong>on</strong>fidence intervals embrace<br />

40,4% and 55,3% of all points, respectively. In equati<strong>on</strong><br />

(4) it corresp<strong>on</strong>ds to R=0,58>R Т (45, 5 %)=0,29, while the<br />

±5% and ±10% c<strong>on</strong>fidence intervals embrace 27,7% and<br />

63,8%, respectively.<br />

We have attempted to describe the annual fluctuati<strong>on</strong> of the<br />

Neman’s water outflow by means of the Markov complex<br />

chain with a shift of 50 years. The regressive analysis of correlati<strong>on</strong>s<br />

defines the particular presentati<strong>on</strong> of the model:<br />

Q(<br />

t ) = 0,<br />

139⋅<br />

Q(<br />

t −1)<br />

+ 0,<br />

195⋅<br />

Q(<br />

t −10<br />

) −<br />

. (5)<br />

− 0,<br />

199⋅<br />

Q(<br />

t − 37 ) + 168,<br />

983 + ξ(<br />

t )<br />

The coefficient of multiple correlati<strong>on</strong> in the equati<strong>on</strong> (5) is<br />

equal to R=0,33>R Т (144, 5%)=0,155, while the ±5% and ±10%<br />

c<strong>on</strong>fidence intervals include 27,1% and 47,9%, respectively,<br />

of all points.<br />

4. C<strong>on</strong>clusi<strong>on</strong>s<br />

This study has shown that there are statistically significant<br />

changes in the dynamics of the annual flow of water in the<br />

Neman river at the stati<strong>on</strong> Grodno within the period of<br />

nearly 200 years investigated here. Changes are influenced<br />

by both natural climate and anthropogenic factors in the hydrological<br />

cycle. Stability of l<strong>on</strong>g-term fluctuati<strong>on</strong>s of the<br />

Neman’s annual flow is observed <strong>on</strong>ly within limited time<br />

intervals of the whole period under investigati<strong>on</strong>. C<strong>on</strong>sidering<br />

the c<strong>on</strong>sistencies of the l<strong>on</strong>g-term fluctuati<strong>on</strong> of the river<br />

annual outflow <strong>on</strong>e needs to apply the methods of c<strong>on</strong>tingent<br />

processes theory, analyze the genesis of the process,<br />

and take into account natural, ec<strong>on</strong>omic and first of all climatic<br />

factors defining its shape.<br />

References<br />

Volchak A.A., Automati<strong>on</strong> of hydrologic calculati<strong>on</strong>s, waterworks<br />

c<strong>on</strong>structi<strong>on</strong> and preservati<strong>on</strong> of the envir<strong>on</strong>ment,<br />

Brest – Nottingham, pp. 55 – 59, 1998.<br />

Ismailov G.H., Fedorov V.M, Analysis of perennial fluctuati<strong>on</strong><br />

of annual flow of Volga, Water Resources, Vol. 28.,<br />

No.5, pp. 517-525, 2001.<br />

Box G.E.P., Jenkins F.M., Time Series Analysis: Forecasting<br />

and C<strong>on</strong>trol, 1 st editi<strong>on</strong>, Mir, Moscow, 1974

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