For an unconfined (water-table) tube well discharging Q with drawdown s through a screen (strainer) of length L and well radius r_w, with radius of influence R, which expression gives the required screen length in terms of aquifer hydraulic conductivity K?
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AL = (Q / (2 * pi * K * s)) * ln(R / r_w)
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BL = (2 * pi * K * s / Q) * ln(R / r_w)
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CL = (Q / (pi * K * s)) * ln(R / r_w)
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DL = (Q / (2 * K * s)) * ln(R / r_w)
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EL = (Q / (2 * pi * K * s)) * (R / r_w)
Answer
Correct Answer: L = (Q / (2 * pi * K * s)) * ln(R / r_w)
Explanation
Introduction / Context:Design of unconfined tube wells requires selecting an adequate screen length to safely pass the target discharge at the allowable drawdown. This uses steady radial-flow relations (Thiem equation) adapted to water-table conditions and distributed inflow along the screen length.
Given Data / Assumptions:
- Unconfined aquifer with hydraulic conductivity K.
- Well radius r_w and radius of influence R (R >> r_w).
- Steady discharge Q with drawdown s at the well under design pumping.
- Uniform inflow along screen length L (first-approximation design).
Concept / Approach:For unconfined flow, the Thiem relation connects discharge to head difference and geometry. Spreading the inflow over the screen length gives an average entrance flux. Rearrangement provides the screen length L necessary to limit entrance flux so that the overall drawdown is s for discharge Q. The commonly used expression is:L = (Q / (2 * pi * K * s)) * ln(R / r_w)with natural logarithm ln().
Step-by-Step Solution:
Start with steady radial flow for unconfined conditions and distribute inflow over L.Relate Q, K, s, and log term ln(R / r_w) from Thiem.Solve for L to obtain: L = (Q / (2 * pi * K * s)) * ln(R / r_w).Verification / Alternative check:Dimensional check: Q has L^3/T; denominator 2 * pi * K * s is L/T; multiplying by the dimensionless ln term yields L (length), as required.
Why Other Options Are Wrong:
- Options with inverted fraction or missing 2 * pi lead to incorrect scaling.
- Replacing ln(R / r_w) with (R / r_w) is incorrect; radial flow solution yields the logarithmic term.
Common Pitfalls:
- Using confined-aquifer formulas directly without adapting to water-table conditions.
- Forgetting the logarithmic dependence on R / r_w.
Final Answer:L = (Q / (2 * pi * K * s)) * ln(R / r_w)