Central Difference Scheme

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Computational methodologies for forced convection
  1. One-Dimensional Steady-State Convection and Diffusion
    1. Central Difference Scheme
    2. Upwind Scheme
    3. Hybrid Scheme
    4. Exponential and Power Law Schemes
    5. A Generalized Expression of Discretization Schemes
  2. Multidimensional Convection and Diffusion Problems
  3. Numerical Solution of Flow Field
    1. Special Difficulties
    2. Staggered grid
    3. Pressure Correction Equation
    4. The SIMPLE Algorithm
  4. Numerical Simulation of Interfaces and Free Surfaces
  5. Application of Computational Methods

Integrating the governing equation over the control volume P (shaded area in Fig. 1), one obtains

Control volume for one-dimensional problem
Figure 1: Control volume for one-dimensional problem.

(\rho u\varphi )_{e}-(\rho u\varphi )_{w}=\left( \Gamma \frac{d\varphi }{dx} \right)_{e}-\left( \Gamma \frac{d\varphi }{dx} \right)_{w}


The right-hand side of eq. (4.211) can be obtained by assuming the distribution of \varphi between any two neighboring grid points is piecewise linear (see Chapter 3), i.e.,

\left( \Gamma \frac{d\varphi }{dx} \right)_{e}=\Gamma _{e}\frac{\varphi _{E}-\varphi _{P}}{(\delta x)_{e}}

\left( \Gamma \frac{d\varphi }{dx} \right)_{w}=\Gamma _{w}\frac{\varphi _{P}-\varphi _{W}}{(\delta x)_{w}}

where Γe and Γw are the diffusivities at the faces of the control volume. To ensure that the flux of \varphi across the faces of the control volume is continuous, the harmonic mean diffusivity at the faces should be used. To evaluate the left hand side of eq. (4.211), it is necessary to know the values of \varphi at the faces of the control volume. If the piecewise linear profile of \varphi is chosen, it follows that

\varphi _{e}=\frac{\varphi _{E}+\varphi _{P}}{2}

\varphi _{w}=\frac{\varphi _{P}+\varphi _{W}}{2}

Therefore, eq. (4.211) becomes

(\rho u)_{e}\frac{\varphi _{E}+\varphi _{P}}{2}-(\rho u)_{w}\frac{\varphi _{P}+\varphi _{W}}{2}=\Gamma _{e}\frac{\varphi _{E}-\varphi _{P}}{(\delta x)_{e}}-\Gamma _{w}\frac{\varphi _{P}-\varphi _{W}}{(\delta x)_{w}}


Defining the mass flux and diffusive conductance

F=\rho u,\text{  }D=\frac{\Gamma }{\delta x}


eq. (4.212) can be rearranged as

a_{P}\varphi _{P}=a_{E}\varphi _{E}+a_{W}\varphi _{W}









This scheme is termed the central difference scheme because the values of \varphi at the faces of the control volume are taken as the averaged value between two grid points. The continuity equation (4.202) requires that Fe = Fw and therefore, eq. (4.217) reduces to

aP = aW + aE

To evaluate the performance of the central difference scheme, let us consider the case of a uniform grid, i.e., x)e = (δx)w = δx, for which case eq. (4.212) can be rearranged as

\varphi _{P}=\frac{1}{2}\left[ \left( 1-\frac{\text{Pe}_{\Delta }}{2} \right)\varphi _{E}+\left( 1+\frac{\text{Pe}_{\Delta }}{2} \right)\varphi _{W} \right]



\text{Pe}_{\Delta }=\frac{\rho u\delta x}{\Gamma }=\frac{F}{D}


is the Peclet number using grid size as the characteristic length, which is referred to as the grid Peclet number. The grid Pe is a ratio of the strength of convection over diffusion. To ensure stability of the discretization scheme, the value of \varphi _{P} should always fall between \varphi _{E} and \varphi _{W}, which requires that the coefficients, \varphi _{E} and \varphi _{W}, are positive, i.e.,

\left| \text{Pe}_{\Delta } \right|\le 2


This is the criterion for stability of the central difference scheme. It can be demonstrated that the central difference becomes unstable if eq. (4.220) is violated (see Problem 4.22). The fact that the central difference scheme is stable under small grid Peclet number indicates that the central difference scheme is accurate only if the convection is not very significant.