Fix typos in examples folder
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@ -67,7 +67,7 @@ timestep 0.0006
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#---------------------------------------------------------------------------
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# Create a lattice-Boltzmann fluid covering the simulation domain.
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# This fluid feels a force due to the particles specified through FluidAtoms
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# (however, this fix does not explicity apply a force back on to these
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# (however, this fix does not explicitly apply a force back on to these
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# particles...this is accomplished through the use of the viscous_lb fix).
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# Use the standard LB integration scheme, a fluid density = 1.0,
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# fluid viscosity = 1.0, lattice spacing dx=0.06, and mass unit, dm=0.00003.
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@ -61,7 +61,7 @@ group FluidAtoms type 2
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#---------------------------------------------------------------------------
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# Create a lattice-Boltzmann fluid covering the simulation domain.
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# This fluid feels a force due to the particles specified through FluidAtoms
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# (however, this fix does not explicity apply a force back on to these
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# (however, this fix does not explicitly apply a force back on to these
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# particles...this is accomplished through the use of the viscous_lb fix).
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# Use the standard LB integration scheme, a fluid viscosity = 1.0, fluid
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# density= 0.0009982071, lattice spacing dx=1.2, and mass unit, dm=0.003.
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@ -61,7 +61,7 @@ group FluidAtoms type 2
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#---------------------------------------------------------------------------
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# Create a lattice-Boltzmann fluid covering the simulation domain.
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# This fluid feels a force due to the particles specified through FluidAtoms
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# (however, this fix does not explicity apply a force back on to these
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# (however, this fix does not explicitly apply a force back on to these
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# particles...this is accomplished through the use of the rigid_pc_sphere
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# fix).
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# Use the LB integration scheme of Ollila et. al. (for stability reasons,
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@ -54,7 +54,7 @@ velocity all set 0.0 0.0 0.0 units box
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#----------------------------------------------------------------------------
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# Create a lattice-Boltzmann fluid covering the simulation domain.
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# All of the particles in the simulation apply a force to the fluid.
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# (however, this fix does not explicity apply a force back on to these
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# (however, this fix does not explicitly apply a force back on to these
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# particles...this is accomplished through the use of the viscous_lb fix.
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# Use the standard LB integration scheme, a fluid density = 1.0,
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# fluid viscosity = 1.0, lattice spacing dx=4.0, and mass unit, dm=10.0.
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@ -54,7 +54,7 @@ velocity all set 0.0 0.0 0.0 units box
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#----------------------------------------------------------------------------
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# Create a lattice-Boltzmann fluid covering the simulation domain.
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# All of the particles in the simulation apply a force to the fluid.
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# (however, this fix does not explicity apply a force back on to these
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# (however, this fix does not explicitly apply a force back on to these
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# particles...this is accomplished through the use of the rigid_pc_sphere
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# fix).
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# Use the LB integration scheme of Ollila et. al. (for stability reasons,
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@ -58,7 +58,7 @@ group FluidAtoms type 2
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#---------------------------------------------------------------------------
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# Create a lattice-Boltzmann fluid covering the simulation domain.
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# This fluid feels a force due to the particles specified through FluidAtoms
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# (however, this fix does not explicity apply a force back on to these
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# (however, this fix does not explicitly apply a force back on to these
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# particles. This is accomplished through the use of the lb/viscous
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# fix).
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# Uses the standard LB integration scheme, fluid viscosity = 0.023333333,
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@ -62,7 +62,7 @@ group FluidAtoms type 2
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#---------------------------------------------------------------------------
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# Create a lattice-Boltzmann fluid covering the simulation domain.
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# This fluid feels a force due to the particles specified through FluidAtoms
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# (however, this fix does not explicity apply a force back on to these
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# (however, this fix does not explicitly apply a force back on to these
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# particles. This is accomplished through the use of the rigid_pc_sphere
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# fix).
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# Use the LB integration scheme of Ollila et. al. (for stability reasons,
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