Knowledge / Civil Engineering / Groundwater hydraulics

Groundwater hydraulics

Civil Engineering (B.E./B.Tech) · Water and environment · free study notes for exams, placements and interviews

In short

Groundwater hydraulics is the study of how water stored in soil and rock moves under a hydraulic gradient, and how much of it a well can safely yield. It rests on Darcy's law and on a small family of well equations (Thiem, Dupuit, Theis, Cooper–Jacob) that convert pumping-test drawdowns into aquifer constants. It matters because about 60–65% of India's irrigation and most of its rural drinking water come from groundwater, and a large number of assessment units are already semi-critical to over-exploited. The topic is examined in GATE Civil (Water Resources / Environmental), in state PSC and ESE papers, and is interviewed at CGWB, state ground water departments, irrigation and minor-irrigation departments, WAPCOS, NABARD-funded well projects, and consultancies doing dewatering, tube-well design and EIA hydrogeology.

Explained

Occurrence of groundwater and types of aquifers

Aquifer properties

MaterialTypical K (m/day)
Gravel100–1,000+
Coarse sand10–100
Fine sand1–10
Silt, loess10⁻³–1
Clay< 10⁻³
Weathered/fractured rock0.1–50 (highly variable)

Darcy's law, its validity and layered ground

Steady radial flow to a well (equilibrium / Thiem theory)

Assumptions (the "Dupuit–Thiem" assumptions): homogeneous, isotropic aquifer of infinite areal extent; fully penetrating well; steady state reached; laminar radial flow; horizontal flow with the gradient equal to the slope of the free surface (small slope); constant discharge.

  1. Confined aquifer: area of flow at radius r is 2πrb; integrate Q = 2πrb K (dh/dr) between two observation wells → Thiem equation. Drawdown varies with log r, so a semi-log plot of s against r is a straight line.
  2. Unconfined aquifer: area is 2πrh (h measured from the impervious base) → Q = πK(h₂² − h₁²)/ln(r₂/r₁). The free surface actually curves above the Dupuit parabola near the well (seepage face), so computed drawdown near the well is in error, but Q is nearly right.
  3. Radius of influence R: distance at which drawdown becomes negligible; it grows with time and is estimated empirically (Sichardt, Kusakin) or by extrapolating the semi-log drawdown line. Typically 100–300 m in fine sand, 300–3,000 m in gravel.
  4. Specific capacity = Q/sw (m³/day per m) — the practical yardstick of a well; it falls as the well ages and screens clog.
  5. Well losses: total drawdown in the well sw = BQ (aquifer/formation loss, laminar) + CQ² (well loss through screen, gravel pack and turbulent entry). Well efficiency = BQ/(BQ + CQ²), found from a step-drawdown test; good wells exceed 70%.
  6. Partial penetration concentrates flow and increases drawdown for the same Q; corrections (Kozeny) or a reduced effective screen length are applied.
  7. Interference: drawdowns of nearby wells superpose (linear for confined aquifers), so the yield per well in a well field is less than for an isolated well — hence minimum spacing norms (commonly 150–300 m for alluvial irrigation tube wells; follow state/CGWB norms).
  8. Boundaries by image wells: an impermeable boundary is simulated by an identical pumping image (drawdown doubles at the boundary); a recharge boundary (river, lake) by a recharging image well (drawdown is cancelled).

Unsteady (non-equilibrium) flow and pumping tests

Wells in Indian practice, management and codes

Key points

Formulas and examples

Darcy: Q = K i A; v = Q/A = K i; seepage velocity vs = v/n (Q m³/day, K m/day, i dimensionless, A m², n porosity)
Validity: Re = ρ v d /μ < 1 (d ≈ d₁₀ effective grain size, m)
Intrinsic permeability k₀ = K μ /(ρ g), m²; Hazen K (cm/s) ≈ C d₁₀² (d₁₀ in cm, C ≈ 100)
T = K b (m²/day); S = Ss b; n = Sy + Sr
Layered: Kh = Σ(Kᵢ zᵢ)/Σzᵢ ; Kv = Σzᵢ / Σ(zᵢ/Kᵢ)
Confined steady (Thiem): Q = 2π T (s₁ − s₂)/ln(r₂/r₁) = 2π K b (h₂ − h₁)/ln(r₂/r₁)
Unconfined steady (Dupuit–Thiem): Q = π K (h₂² − h₁²)/ln(r₂/r₁) = π K (H² − hw²)/ln(R/rw)
Theis: s = (Q/4πT) W(u), u = r² S /(4 T t); W(u) = −0.5772 − ln u + u − u²/4 + …
Cooper–Jacob: s = (2.303 Q /4πT) log₁₀(2.25 T t /(r² S)); T = 2.303 Q /(4π Δs per log cycle); S = 2.25 T t₀ /r²
Recovery: s′ = (2.303 Q /4πT) log₁₀(t/t′) (t from start of pumping, t′ from stopping)
Well drawdown: sw = B Q + C Q²; specific capacity = Q/sw; well efficiency = BQ/sw
Radius of influence (Sichardt, approximate): R = 3000 s √K, with s in m and K in m/s
Open well recuperation: C = K/A = (2.303/t) log₁₀(h₁/h₂); safe yield Q = C·A·H (A = plan area m², H = working depression head m, C per hour)
Ghyben–Herzberg: hs = [ρf/(ρs − ρf)] hf ≈ 40 hf (hf = freshwater head above MSL)
Stage of ground water extraction (%) = 100 × annual extraction / annual extractable resource

Example 1 – Darcy's law, transmissivity and seepage velocity. A confined sand aquifer is 25 m thick, K = 30 m/day, porosity 0.25, and the piezometric surface falls 1 m in 200 m.

Example 2 – Thiem test on a confined aquifer (T, K, specific capacity). A fully penetrating well in a 20 m thick confined aquifer is pumped at a steady 1,800 m³/day. Drawdown is 3.0 m at r = 10 m and 1.2 m at r = 100 m.

Example 3 – Dupuit equation for an unconfined aquifer. Unconfined aquifer, K = 25 m/day, initial saturated depth H = 30 m above the impervious base. A 30 cm diameter well is pumped until the water depth in it is 24 m, with R = 300 m.

Example 4 – Cooper–Jacob prediction of drawdown. Confined aquifer, T = 500 m²/day, S = 2 × 10⁻⁴. A well pumps 1,500 m³/day. Find the drawdown at r = 50 m after 1 day.

Example 5 – Open well recuperation test (Indian practice). A 2 m diameter open well is depressed 2.5 m below the static level by pumping; in 90 minutes the level recuperates by 1.8 m.

FeatureConfined aquiferUnconfined aquifer
Upper boundaryImpervious layerWater table
Water released byCompression of matrix, expansion of waterGravity drainage of pores
S10⁻⁵ – 10⁻³0.05 – 0.30 (≈ Sy)
TKb, constantKh, falls as level drops
Steady equationQ ∝ (h₂ − h₁)Q ∝ (h₂² − h₁²)
Cone of depressionSpreads fast and far, little dewateringSpreads slowly, actual dewatering
RechargeOnly through the outcrop/leakageDirect vertical infiltration
MethodNeedsGivesBest for
Thiem (steady)2 observation wells, steady stateT, KLong-pumped alluvial wells
Theis type curves–t data, one obs. wellT and SConfined, early-time data
Cooper–Jacobs vs log t straight lineT and SRoutine field analysis, u < 0.01
Recovery testResidual drawdown after stoppingTWhen discharge is unsteady
Step-drawdown3–5 steps of increasing QB, C, efficiencyWell performance, pump selection
RecuperationSingle open wellC (= K/A), safe yieldDug wells in hard rock

Where it is used

Interview questions

Common mistakes

Related topics

Hydrology · Irrigation engineering · Water supply engineering · Rainwater harvesting and water conservation · Fluid properties and statics · Seepage and permeability in soil mechanics

Open in the Knowledge reader →Find jobs →