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RESEARCH· ·1970·

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B220<br />

RELATION· BETWEEN GROUND<br />

erally prevail. In extended dry periods, however, the<br />

water level drops below the confining layer of silt and<br />

clay.·<br />

Four observation wells, consisting of 2-inch pipe<br />

with 60-gauze screen set approximately 9 feet below<br />

land surface, were installed on line with the gage and<br />

perpendicular to the river. Elevations referenced to<br />

existing gage datum were determined for each well.<br />

After the site was chosen and the observation ·wells<br />

were installed, periodic measurements of water level<br />

were· made to define the direction of subsurface flow.<br />

Measurements were made during floods in the late winter<br />

and spring of 1968. Analyses of the exchange<br />

mechanism for three peaks which occurred are discussed.<br />

The stream-stage hydrographs for one relatively<br />

small peak, one medium peak, and one relatively<br />

high peak (overbank) are shown in figure 2.<br />

METHODS AND RESULTS ·OF STUDY<br />

The method used in the analysis of these peaks will<br />

be illustrated using peak 3 of figure 2. Potentiometric<br />

profiles for stages A -E are shown in figure 3.<br />

Under recession conditions (stage .A.), ground-water<br />

movement is toward and into the stream. As the stream<br />

level rises above the water level in the adjacent aquifer<br />

(stage B) the hydraulic gradient at the interface is reversed<br />

and water moves from the stream into the<br />

banks. Immediately after the beginning of the rise,<br />

therefore, the discharge of ground water into the<br />

stream ceases. However, ground water continues to<br />

move from the valley margins toward the stream, but<br />

its progress is blocked by the opposing gradient. As<br />

a result, the amount of ground water that would normally<br />

have been discharged into the stream is tempo-<br />

14<br />

13<br />

12<br />

t;j<br />

l.lJ 11<br />

L&..<br />

z<br />

~ 10<br />

:I:<br />

(!)<br />

ijj 9<br />

:I:<br />

w<br />

(!) 8<br />

<<br />

(!)<br />

6<br />

Peak 1<br />

----- Bankfull stage<br />

Time .at which potentiometric{A 8<br />

C<br />

0<br />

E<br />

prof1les were made for stages 1 1 1 1 1<br />

A-E. Profiles shown on figure<br />

3<br />

50 100 150 200 250 0 50 100 150 0 50 100 150<br />

Began 1800 hours<br />

January 27, 1968<br />

Began 1530 hours<br />

March 24, 1968<br />

Began 1700 hours<br />

April 3, 1968<br />

TIME, IN HOURS<br />

E'muRE 2.~Stream-stage hydrographs for three storm-peak flows<br />

in winter and .spring of 1968.<br />

WATER AND SURFACE WATER<br />

13 Land surface<br />

4 3<br />

12 Well number<br />

11<br />

l.lJ<br />

(!)<br />

<<br />

(!) 7<br />

6<br />

13<br />

12<br />

t;j 11<br />

l.lJ<br />

L&..<br />

~ 10<br />

~<br />

a 9<br />

ijj<br />

J:<br />

w 8<br />

(!)<br />

<<br />

(!) 7<br />

6<br />

0 100 200 300 400 500 600 700 800 900 1000 1100 1200<br />

HORIZONTAL DISTANCE, IN FEET<br />

Land surface<br />

I<br />

4 3 2 Gage<br />

Well number<br />

Silt and clay<br />

----------------~--~<br />

Sand<br />

'-<br />

0 100 200 300 400 500 600 700 800 900 1000 1100 1200<br />

HORIZONTAL DISTANCE, IN FEET<br />

FIGURE 3.-Potentiometric profiles of storm peak 3 (fig. 2) at<br />

stages and times shown on figure 2. Arrows indicate flow<br />

direction.<br />

rarily s'tored. This is indicated by corresponding rises<br />

in the water level in the observation wells (stage 0).<br />

Soon after the peak stream stage, the water in bank<br />

storage (Langbein and Iseri, 1960) begins to move<br />

back into the stream. At stage E, a gradient toward<br />

the stream has been reestablished throughout the<br />

section.<br />

A convenient method for analyzing the volumetric<br />

exchange of water between the stream and the ground<br />

is by use of Darcy's law. It is stated mathematically<br />

as the equation.<br />

Q=TiL,<br />

(1)<br />

where<br />

Q= dischar~e,<br />

T~ transmissivity,<br />

i =hydraulic gradient, and<br />

L==width of section. ·<br />

But<br />

v<br />

Q=-,<br />

(2)<br />

t<br />

., '<br />

""'<br />

·~!<br />

~' "·

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