Hydraulic Fracturing Overview

Introduction

Hydraulic fracturing is a well stimulation technique that creates conductive flow channels in the reservoir rock by injecting fluid at pressures exceeding the formation fracture gradient. The induced fracture dramatically increases the effective wellbore contact area, enabling economic production from formations that would otherwise be unproductive.

Petroleum Office provides analytical models for fracture geometry prediction, leakoff analysis, and proppant transport calculations covering the classical 2D fracture models and supporting design computations.

Why Hydraulic Fracturing?

Hydraulic fracturing is performed when the natural reservoir deliverability is insufficient for economic production:

  • Low permeability -- tight sandstones, shales, and carbonates where matrix flow is too slow
  • Near-wellbore damage -- drilling damage (positive skin) that restricts inflow
  • Thin pay zones -- limited productive interval requiring enhanced contact area
  • Bypassing heterogeneity -- reaching past near-wellbore barriers to undamaged rock

The Skin Analogy

An unfractured damaged well has a positive skin factor S>0S > 0 that reduces productivity. A hydraulic fracture creates an equivalent negative skin, dramatically increasing effective wellbore radius:

rw=rweSr_w' = r_w e^{-S}

For a propped fracture of half-length xfx_f and finite conductivity FcDF_{cD}, the equivalent skin can reach S=4S = -4 to 6-6, corresponding to effective wellbore radii tens to hundreds of times larger than the physical wellbore.


Fracture Geometry Fundamentals

How a Fracture Propagates

When fluid is injected above the fracture pressure:

                    Injection
                       │
                       ▼
        ┌──────────────┬──────────────┐
        │              │              │  Overburden
        ├──────────────┼──────────────┤  ─── Stress Barrier (upper)
        │     ◄────────┼────────►     │
        │   Fracture   │  Fracture    │  Pay Zone
        │     wing     │   wing       │  (height h)
        ├──────────────┼──────────────┤  ─── Stress Barrier (lower)
        │              │              │  Underburden
        └──────────────┴──────────────┘

              xf             xf
        ◄──────────►  ◄──────────►
           Half-length    Half-length

The fracture propagates as a bi-wing crack extending symmetrically from the wellbore. The geometry -- width, length (or radius), and height -- depends on the balance between:

  1. Fluid pressure inside the fracture
  2. In-situ stress resisting fracture opening
  3. Rock stiffness (Young's modulus) resisting deformation
  4. Fluid leakoff into the formation walls

Key Geometric Parameters

Parameter Symbol Description Typical Range
Half-length xfx_f Distance from wellbore to fracture tip 100 -- 2,000 ft
Width ww Fracture opening (aperture) 0.1 -- 1.0 in
Height hfh_f Vertical extent of fracture 20 -- 300 ft
Radius RR Radial extent (penny-shaped model) 100 -- 1,000 ft
Net pressure pnetp_{net} Fluid pressure minus closure stress 100 -- 2,000 psi

2D Fracture Geometry Models

Three classical analytical models describe fracture geometry under different assumptions about height confinement and deformation mode:

Model Overview

    PKN Model              KGD Model            Radial Model
    (confined height)      (confined height)    (unconfined)

    ┌────────────┐         ┌────────────┐
    │  │         │         │            │           ╱  ╲
    │  │ ellipse │         │ rectangle  │         ╱      ╲
    │  │ cross-  │         │ cross-     │       ╱    ●     ╲
    │  │ section │         │ section    │         ╲      ╱
    │  │         │         │            │           ╲  ╱
    └────────────┘         └────────────┘        penny-shaped

    w varies along L       w uniform along h     w varies with R
    w_max at wellbore      w_max at center       w_max at center
    Plane strain: vert.    Plane strain: horiz.  Axial symmetry

Decision Guide: PKN vs KGD vs Radial

Factor PKN KGD Radial
Height confinement Strong barriers Strong barriers No barriers
Length vs height xfhfx_f \gg h_f xfhfx_f \leq h_f No fixed height
Plane strain Vertical Horizontal Axial symmetry
Width maximum At wellbore At center of length At center
Net pressure trend Increases with time Decreases with time Decreases with time
Best application Long fractures in bounded pay Short/wide fractures Early time, thick zones
Typical use Most common design model Lab-scale, short fracs Radial propagation phase

Rule of thumb:

  • If xf/hf>1x_f / h_f > 1 (fracture longer than tall): PKN
  • If xf/hf<1x_f / h_f < 1 (fracture shorter than tall): KGD
  • If height is unconstrained: Radial

Detailed Documentation


Leakoff and Fluid Efficiency

Carter Leakoff Model

Not all injected fluid goes into creating fracture volume. A significant portion leaks off into the permeable formation walls. Carter (1957) described the leakoff velocity as:

uL=CLtτu_L = \frac{C_L}{\sqrt{t - \tau}}

Where:

  • uLu_L = leakoff velocity, ft/min
  • CLC_L = total leakoff coefficient, ft/min$^{1/2}$
  • tt = current time
  • τ\tau = time at which the fracture face was first exposed

Three Leakoff Mechanisms

Mechanism Coefficient Controlled By
Viscous wall-building CIC_I Filter-cake resistance
Reservoir filtrate CIIC_{II} Formation permeability and viscosity
Compressibility CIIIC_{III} Reservoir compressibility and pressure

The total leakoff coefficient combines all three:

1CL=1CI+1CII+1CIII\frac{1}{C_L} = \frac{1}{C_I} + \frac{1}{C_{II}} + \frac{1}{C_{III}}

Fluid Efficiency

Fluid efficiency (η\eta) is the fraction of injected volume that remains in the fracture at any time:

η=VfracVinjected\eta = \frac{V_{frac}}{V_{injected}}

Efficiency Range Leakoff Character Formation Type
η>0.7\eta > 0.7 Low leakoff Tight rock, good fluid
0.3<η<0.70.3 < \eta < 0.7 Moderate leakoff Moderate permeability
η<0.3\eta < 0.3 High leakoff High permeability, poor fluid

Fluid efficiency directly affects fracture dimensions -- higher leakoff means shorter, narrower fractures for the same injection volume.

Detailed Documentation


Proppant Transport

Purpose

After pumping stops, the induced fracture closes under in-situ stress. Proppant (sand, ceramic beads, or resin-coated particles) is placed inside the fracture during the treatment to keep it propped open, maintaining a conductive flow path from the reservoir to the wellbore.

Key Considerations

                Fracture Width (w)
                ◄─────────────►
    ┌───────────────────────────────────┐
    │  ○ ○   ○  ○ ○  ○   ○  ○  ○  ○   │  ▲
    │ ○  ○ ○  ○   ○  ○ ○  ○  ○  ○  ○  │  │
    │  ○  ○ ○  settling  ○  ○  ○   ○   │  │  Fracture
    │   ○ ○  ▼  ○ ○  ○ ○   ○  ○ ○  ○  │  │  Height
    │ ○  ○ ○  ○  ○ ○  ○  ○  ○  ○ ○  ○ │  │  (h)
    │○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ ○ │  │
    │○○○○○○○○○○○○○○○○○○○○○○○○○○○○○○○○│  ▼
    └───────────────────────────────────┘
           Proppant bank (settled)

Proppant settling during pumping determines the final proppant distribution:

  • Settling velocity depends on particle size, density contrast, and fluid rheology
  • Wall effects slow settling when particles are large relative to fracture width
  • Concentration effects reduce settling in dense slurries (hindered settling)
  • Fluid rheology -- power-law fluids used in fracturing significantly reduce settling

Transport Ratio

The transport ratio compares horizontal proppant velocity to settling velocity, indicating whether proppant reaches the fracture tip or banks near the wellbore.

Detailed Documentation

  • Proppant Transport -- Settling velocity, wall effects, hindered settling, power-law corrections

Available Calculation Categories

Fracture Geometry

Category Description Functions
PKN Model Width, length, pressure, volume for confined long fractures Width, length (no-loss and leakoff), net pressure, volume
KGD Model Width, length, pressure, volume for confined short fractures Width, length (no-loss), net pressure, volume
Radial Model Width, radius, pressure, volume for unconfined fractures Width, radius (no-loss), net pressure
Leakoff Carter leakoff velocity, cumulative volume, fluid efficiency Velocity, cumulative loss, efficiency

Proppant Transport

Category Description Functions
Settling Stokes, field (corrected), and hindered settling velocities Multiple settling models
Corrections Wall effects, concentration effects, power-law fluids Correction factors
Transport Settling distance, transport ratio, particle Reynolds number Design parameters

Practical Workflow

Step 1: Characterize the Formation

  1. Determine in-situ stress profile (closure stress, barriers)
  2. Obtain rock mechanical properties (Young's modulus, Poisson's ratio)
  3. Assess formation permeability and leakoff potential
  4. Define pay zone thickness and barrier locations

Step 2: Select Geometry Model

Loading diagram...

Step 3: Estimate Leakoff

  1. Determine leakoff coefficient from mini-frac or lab data
  2. Calculate fluid efficiency for the planned pump rate and volume
  3. Adjust treatment volume to achieve target fracture dimensions

Step 4: Design Proppant Placement

  1. Calculate settling velocity for chosen proppant and fluid
  2. Assess transport ratio -- will proppant reach the tip?
  3. Determine proppant concentration schedule
  4. Verify fracture width exceeds 3x proppant diameter for placement

Step 5: Predict Fracture Dimensions

  1. Calculate width, length/radius, and net pressure
  2. Verify fracture stays within target zone (height containment)
  3. Estimate propped fracture conductivity
  4. Calculate equivalent skin and productivity improvement

Fracture Models and Proppant

Production Impact

Rock and Fluid Properties

  • PVT Overview -- Fluid property correlations for leakoff calculations

References

  1. Economides, M.J. and Nolte, K.G. (2000). Reservoir Stimulation, 3rd Edition. John Wiley & Sons.

  2. Valko, P. and Economides, M.J. (1995). Hydraulic Fracture Mechanics. John Wiley & Sons.

  3. Carter, R.D. (1957). "Derivation of the General Equation for Estimating the Extent of the Fractured Area." Appendix to: Howard, G.C. and Fast, C.R., "Optimum Fluid Characteristics for Fracture Extension." Drilling and Production Practice, API, pp. 261-270.

  4. Perkins, T.K. and Kern, L.R. (1961). "Widths of Hydraulic Fractures." Journal of Petroleum Technology, 13(9), pp. 937-949. SPE-89-PA.

  5. Geertsma, J. and de Klerk, F. (1969). "A Rapid Method of Predicting Width and Extent of Hydraulically Induced Fractures." Journal of Petroleum Technology, 21(12), pp. 1571-1581. SPE-2458-PA.

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