|
|
Line 1: |
Line 1: |
| The '''Oldroyd-B model''' is a constitutive model used to describe the flow of [[viscoelastic]] fluids.
| | I'm Roy and I live in Kommel. <br>I'm interested in Occupational Therapy, American football and Dutch art. I like travelling and reading fantasy.<br><br>Here is my homepage bola terpercaya ([http://www.quesadasolidaria.org/web/guest/36/-/blogs/el-testimonio-de-un-voluntario;jsessionid=90cc08737857130a9645678e700e209d?_33_redirect=/web/guest/36/-/blogs& pop over to this website]) |
| This model can be regarded as an extension of the [[Upper Convected Maxwell model]] and is equivalent to a fluid filled with elastic bead and spring dumbbells.
| |
| The model is named after its creator [[James G. Oldroyd]].
| |
| | |
| The model can be written as:
| |
| :<math> \mathbf{T} + \lambda_1 \stackrel{\nabla}{\mathbf{T}} = 2\eta_0 (\mathbf{D} + \lambda_2 \stackrel{\nabla}{\mathbf{D}}) </math>
| |
| where:
| |
| * <math>\mathbf{T}</math> is the [[Stress (physics)|stress]] [[tensor]];
| |
| * <math>\lambda_1</math> is the relaxation time;
| |
| * <math>\lambda_2</math> is the retardation time = <math> \frac{\eta_s}{\eta_0}\lambda_1 </math>;
| |
| * <math> \stackrel{\nabla}{\mathbf{T}} </math> is the [[Upper convected time derivative]] of stress tensor:
| |
| :<math> \stackrel{\nabla}{\mathbf{T}} = \frac{\partial}{\partial t} \mathbf{T} + \mathbf{v} \cdot \nabla \mathbf{T} -( (\nabla \mathbf{v})^T \cdot \mathbf{T} + \mathbf{T} \cdot (\nabla \mathbf{v})) </math>;
| |
| *<math>\mathbf{v}</math> is the fluid velocity;
| |
| *<math>\eta_0</math> is the total [[viscosity]] composed of solvent and polymer components, <math> \eta_0= \eta_s + \eta_p </math>;
| |
| *<math>\mathbf {D}</math> is the deformation rate tensor or rate of strain tensor, <math>\mathbf{D} = \frac{1}{2}\left[\boldsymbol\nabla \mathbf{v} + (\boldsymbol\nabla \mathbf{v})^T\right]</math>.
| |
| | |
| The model can also be written split into polymeric (viscoelastic) part separately from the solvent part:
| |
| <math> \mathbf{T} = 2\eta_s \mathbf{D} + \mathbf{\tau} </math>.
| |
| | |
| where
| |
| :<math> \mathbf{\tau} + \lambda_1 \stackrel{\nabla}{\mathbf{\tau}} = 2\eta_p \mathbf{D} </math>
| |
| | |
| | |
| | |
| | |
| Whilst the model gives good approximations of viscoelastic fluids in shear flow, it has an unphysical singularity in extensional flow, where the dumbbells are infinitely stretched;
| |
| If the solvent viscosity is zero then the Oldroyd-B becomes the [[Upper Convected Maxwell model]].
| |
| | |
| | |
| ==References==
| |
| * {{cite journal|last=Oldroyd|first=James|title=On the Formulation of Rheological Equations of State|journal=Proceedings of the Royal Society of London. Series A, Mathematical and Physical Sciences|year=1950|month=Feb|volume=200|issue=1063|pages=523–541}}
| |
| | |
| * {{cite book | author=Owens, R. G.,Phillips, T. N.| title=Computational Rheology.| publisher=Imperial College Press | year=2002 | isbn=978-1-86094-186-3}}
| |
| | |
| [[Category:Non-Newtonian fluids]]
| |
I'm Roy and I live in Kommel.
I'm interested in Occupational Therapy, American football and Dutch art. I like travelling and reading fantasy.
Here is my homepage bola terpercaya (pop over to this website)