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The | In [[mathematics]], the '''Courant–Friedrichs–Lewy condition''' (CFL condition) is a necessary condition for [[Numerical stability#Stability in numerical differential equations|stability]] while solving certain [[partial differential equation]]s (usually [[Hyperbolic partial differential equation|hyperbolic PDE]]s) numerically by the [[Finite difference method|method of finite differences]].<ref>In general, it is not a sufficient condition; also, it can be a demanding condition for some problems. See the "[[Courant–Friedrichs–Lewy condition#Implications of the CFL condition|Implications of the CFL condition]]" section of this article for a brief survey of these issues.</ref> It arises in the [[numerical analysis]] of [[explicit method|explicit]] time-marching schemes, when these are used for the numerical solution. As a consequence, the time step must be less than a certain time in many [[explicit method|explicit]] time-marching [[computer simulation]]s, otherwise the simulation will produce incorrect results. The condition is named after [[Richard Courant]], [[Kurt Friedrichs]], and [[Hans Lewy]] who described it in their 1928 paper.<ref>See reference {{harvnb|Courant|Friedrichs|Lewy|1928}}. There exists also an [[English language|English]] [[translation]] of the 1928 [[German language|German]] original: see references {{harvnb|Courant|Friedrichs|Lewy|1956}} and {{harvnb|Courant|Friedrichs|Lewy|1967}}.</ref> | ||
This condition is an example of [[temporal discretization|explicit time integration]] where the function that defines governing equation is evaluated at the current time.{{clarify|reason=What does {{''}}evaluated at the current time{{''}} mean? And what does {{''}}current time{{''}} refer to? What does it mean that the CFL condition is an {{''}}example{{''}} of explicit time integration? Isn't it rather be a restriction?|date=November 2013}} | |||
==Heuristic description== | |||
The principle behind the condition is that, for example, if a wave is moving across a discrete spatial grid and we want to compute its [[amplitude]] at discrete time steps of equal length,<ref>This situation commonly occurs when a [[hyperbolic partial differential equation|hyperbolic partial differential operator]] has been [[approximation theory|approximated]] by a [[Finite difference|finite difference equation]], which is then solved by [[numerical linear algebra]] methods.</ref> then this length must be less than the time for the wave to travel to adjacent grid points. As a corollary, when the grid point separation is reduced, the upper limit for the time step also decreases. In essence, the numerical domain of dependence of any point in space and time (which data values in the initial conditions affect the numerical computed value at that point) must include the analytical domain of dependence (where in the initial conditions has an effect on the exact value of the solution at that point) in order to assure that the scheme can access the information required to form the solution. | |||
==The CFL condition== | |||
In order to make a reasonably formally precise statement of the condition, it is necessary to define the following quantities | |||
*''Spatial coordinate'': it is one of the [[coordinate]]s of the [[physical space]] in which the problem is posed. | |||
*''Spatial dimension of the problem'': it is the number <math>n</math> of [[Dimension (mathematics)|spatial dimensions]] i.e. the number of spatial [[coordinate]]s of the [[physical space]] where the problem is posed. Typical values are <math>n=1</math>, <math>n=2</math> and <math>n=3</math>. | |||
*''Time'': it is the [[coordinate]], acting as a [[parameter]], which describes the evolution of the system, distinct from the spatial coordinates. | |||
The spatial coordinates and the time are supposed to be discrete-valued independent [[Variable (mathematics)|variables]], which are placed at regular distances called the ''interval length''<ref>This quantity is not necessarily the same for each spatial variable, as it is shown in the "[[Courant–Friedrichs–Lewy condition#The two and general ''n''–dimensional case|The two and general ''n''–dimensional case]]" section of this entry : it can be chosen in order to somewhat relax the condition.</ref> and the ''time step'', respectively. Using these names, the CFL condition relates the length of the time step to a function of the interval lengths of each spatial coordinate and of the maximum speed with which information can travel in the physical space. | |||
Operatively, the CFL condition is commonly prescribed for those terms of the [[finite-difference approximation]] of general [[partial differential equation]]s which model the [[advection]] phenomenon.<ref>Precisely, this is the hyperbolic part of the PDE under analysis.</ref> | |||
===The one-dimensional case=== | |||
For one-dimensional case, the CFL has the following form: | |||
: <math>C = \frac {u\,\Delta t} {\Delta x} \leq C_{max} </math> | |||
where the [[dimensionless number]] is called the '''Courant number''', | |||
*<math>u</math> is the [[Magnitude (mathematics)|magnitude]] of the velocity (whose [[Dimensional analysis#Definition|dimension]] is length/time) | |||
*<math>\Delta t</math> is the time step (whose [[Dimensional analysis#Definition|dimension]] is time) | |||
*<math>\Delta x</math> is the length interval (whose [[Dimensional analysis#Definition|dimension]] is length). | |||
The value of <math>C_{max}</math> changes with the method used to solve the discretised equation, especially depending on whether the method is [[Explicit and implicit methods|explicit or implicit]]. If an explicit (time-marching) solver is used then typically <math>C_{max} = 1</math>. Implicit (matrix) solvers are usually less sensitive to numerical instability and so larger values of <math>C_{max}</math> may be tolerated. | |||
===The two and general ''n''-dimensional case=== | |||
In the [[Dimension (mathematics)|two-dimensional]] case, the CFL condition becomes | |||
:<math>C = \frac {u_ x\,\Delta t}{\Delta x} + \frac {u_ y\,\Delta t}{\Delta y} \leq C_{max} </math> | |||
with obvious meaning of the symbols involved. By analogy with the two-dimensional case, the general CFL condition for the <math>n</math>-dimensional case is the following one: | |||
:<math>C = \Delta t \sum_{i=1}^n\frac{u_{x_i}}{\Delta x_i} \leq C_{max}. </math> | |||
The interval length is not required to be the same for each spatial variable <math>\Delta x_i, i = 1, ..., n</math>. This "[[Degrees of freedom (physics and chemistry)|degree of freedom]]" can be used in order to somewhat optimize the value of the time step for a particular problem, by varying the values of the different interval in order to keep it not too small. | |||
==Implications of the CFL condition== | |||
===The CFL condition is only a necessary one=== | |||
The CFL condition is a necessary condition, but may not be sufficient for the convergence of the [[finite-difference approximation]] of a given [[numerical method|numerical problem]]. Thus, in order to establish the convergence of the finite-difference approximation, it is necessary to use other methods, which in turn could imply further limitations on the length of the time step and/or the lengths of the spatial intervals. | |||
===The CFL condition can be a very strong requirement=== | |||
The CFL condition can be a very limiting constraint on the time step <math>\Delta t</math>: for example, in the [[finite-difference approximation]] of certain fourth-order nonlinear partial differential equations, it can have the following form:{{fact|date=November 2013}} | |||
: <math>\frac{\Delta t}{(\Delta x)^4} < C u</math> | |||
meaning that a decrease in the length interval <math>\Delta x</math> requires a fourth order decrease in the time step <math>\Delta t</math> for the condition to be fulfilled. Therefore, when solving particularly stiff problems, efforts are often made to avoid the CFL condition, for example by using [[implicit method]]s. | |||
== Notes == | |||
{{reflist|30em}} | |||
== References == | |||
*{{Citation | |||
| last = Courant | |||
| first = R. | |||
| author-link = Richard Courant | |||
| last2 = Friedrichs | |||
| first2 = K. | |||
| author2-link = Kurt Otto Friedrichs | |||
| last3 = Lewy | |||
| first3 = H. | |||
| author3-link = Hans Lewy | |||
| title = Über die partiellen Differenzengleichungen der mathematischen Physik | |||
| journal = [[Mathematische Annalen]] | |||
| volume = 100 | |||
| issue = 1 | |||
| pages = 32–74 | |||
| year = 1928 | |||
| month = | |||
| language = [[German language|German]] | |||
| url = http://resolver.sub.uni-goettingen.de/purl?GDZPPN002272636 | |||
| doi = 10.1007/BF01448839 | |||
| jfm = 54.0486.01 | |||
| mr = 1512478 | |||
|bibcode = 1928MatAn.100...32C }}. | |||
*{{Citation | |||
| last = Courant | |||
| first = R. | |||
| author-link = Richard Courant | |||
| last2 = Friedrichs | |||
| first2 = K. | |||
| author2-link = Kurt Otto Friedrichs | |||
| last3 = Lewy | |||
| first3 = H. | |||
| author3-link = Hans Lewy | |||
| title = On the partial difference equations of mathematical physics | |||
| place = New York | |||
| publisher = AEC Computing and Applied Mathematics Centre – [[Courant Institute of Mathematical Sciences]] | |||
| series = AEC Research and Development Report | |||
| volume = NYO-7689 | |||
| origyear = 1928 | |||
| year = 1956 | |||
| month= September | |||
| edition = | |||
| pages = V + 76 | |||
| language = | |||
| url = http://www.archive.org/details/onpartialdiffere00cour | |||
| archiveurl = http://www.archive.org/stream/onpartialdiffere00cour#page/n0/mode/2up | |||
| archivedate = October 23, 2008 | |||
| doi = | |||
| id = | |||
| isbn = | |||
}}.: translated from the [[German language|German]] by Phyllis Fox. This is an earlier version of the paper {{harvnb|Courant|Friedrichs|Lewy|1967}}, circulated as a research report. | |||
*{{Citation | |||
| last = Courant | |||
| first = R. | |||
| author-link = Richard Courant | |||
| last2 = Friedrichs | |||
| first2 = K. | |||
| author2-link = Kurt Otto Friedrichs | |||
| last3 = Lewy | |||
| first3 = H. | |||
| author3-link = Hans Lewy | |||
| title = On the partial difference equations of mathematical physics | |||
| journal = [http://researchweb.watson.ibm.com/journal/rdindex.html IBM Journal of Research and Development] | |||
| volume = 11 | |||
| issue = 2 | |||
| pages = 215–234 | |||
| origyear = 1928 | |||
| year = 1967 | |||
| month = March | |||
| url = http://domino.research.ibm.com/tchjr/journalindex.nsf/a3807c5b4823c53f85256561006324be/769774a3c9f3685f85256bfa00683f8a!OpenDocument | |||
| mr = 0213764 | |||
| zbl = 0145.40402 | |||
}}. A freely downlodable copy can be found [http://www.stanford.edu/class/cme324/classics/courant-friedrichs-lewy.pdf here]. | |||
== External links == | |||
*{{springer | |||
| title=Courant–Friedrichs–Lewy condition | |||
| id= C/c026760 | |||
| last= Bakhvalov | |||
| first= N. S. | |||
| author-link= Nikolai Sergeevich Bakhvalov | |||
}} | |||
*{{MathWorld |title=Courant-Friedrichs-Lewy Condition |id=Courant-Friedrichs-LewyCondition}} | |||
{{DEFAULTSORT:Courant-Friedrichs-Lewy condition}} | |||
[[Category:Numerical differential equations]] | |||
[[Category:Computational fluid dynamics]] |
Revision as of 01:19, 27 September 2013
In mathematics, the Courant–Friedrichs–Lewy condition (CFL condition) is a necessary condition for stability while solving certain partial differential equations (usually hyperbolic PDEs) numerically by the method of finite differences.[1] It arises in the numerical analysis of explicit time-marching schemes, when these are used for the numerical solution. As a consequence, the time step must be less than a certain time in many explicit time-marching computer simulations, otherwise the simulation will produce incorrect results. The condition is named after Richard Courant, Kurt Friedrichs, and Hans Lewy who described it in their 1928 paper.[2] This condition is an example of explicit time integration where the function that defines governing equation is evaluated at the current time.Template:Clarify
Heuristic description
The principle behind the condition is that, for example, if a wave is moving across a discrete spatial grid and we want to compute its amplitude at discrete time steps of equal length,[3] then this length must be less than the time for the wave to travel to adjacent grid points. As a corollary, when the grid point separation is reduced, the upper limit for the time step also decreases. In essence, the numerical domain of dependence of any point in space and time (which data values in the initial conditions affect the numerical computed value at that point) must include the analytical domain of dependence (where in the initial conditions has an effect on the exact value of the solution at that point) in order to assure that the scheme can access the information required to form the solution.
The CFL condition
In order to make a reasonably formally precise statement of the condition, it is necessary to define the following quantities
- Spatial coordinate: it is one of the coordinates of the physical space in which the problem is posed.
- Spatial dimension of the problem: it is the number of spatial dimensions i.e. the number of spatial coordinates of the physical space where the problem is posed. Typical values are , and .
- Time: it is the coordinate, acting as a parameter, which describes the evolution of the system, distinct from the spatial coordinates.
The spatial coordinates and the time are supposed to be discrete-valued independent variables, which are placed at regular distances called the interval length[4] and the time step, respectively. Using these names, the CFL condition relates the length of the time step to a function of the interval lengths of each spatial coordinate and of the maximum speed with which information can travel in the physical space.
Operatively, the CFL condition is commonly prescribed for those terms of the finite-difference approximation of general partial differential equations which model the advection phenomenon.[5]
The one-dimensional case
For one-dimensional case, the CFL has the following form:
where the dimensionless number is called the Courant number,
- is the magnitude of the velocity (whose dimension is length/time)
- is the time step (whose dimension is time)
- is the length interval (whose dimension is length).
The value of changes with the method used to solve the discretised equation, especially depending on whether the method is explicit or implicit. If an explicit (time-marching) solver is used then typically . Implicit (matrix) solvers are usually less sensitive to numerical instability and so larger values of may be tolerated.
The two and general n-dimensional case
In the two-dimensional case, the CFL condition becomes
with obvious meaning of the symbols involved. By analogy with the two-dimensional case, the general CFL condition for the -dimensional case is the following one:
The interval length is not required to be the same for each spatial variable . This "degree of freedom" can be used in order to somewhat optimize the value of the time step for a particular problem, by varying the values of the different interval in order to keep it not too small.
Implications of the CFL condition
The CFL condition is only a necessary one
The CFL condition is a necessary condition, but may not be sufficient for the convergence of the finite-difference approximation of a given numerical problem. Thus, in order to establish the convergence of the finite-difference approximation, it is necessary to use other methods, which in turn could imply further limitations on the length of the time step and/or the lengths of the spatial intervals.
The CFL condition can be a very strong requirement
The CFL condition can be a very limiting constraint on the time step : for example, in the finite-difference approximation of certain fourth-order nonlinear partial differential equations, it can have the following form:Template:Fact
meaning that a decrease in the length interval requires a fourth order decrease in the time step for the condition to be fulfilled. Therefore, when solving particularly stiff problems, efforts are often made to avoid the CFL condition, for example by using implicit methods.
Notes
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References
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In case you are in search of an actual estate or Singapore property agent on-line, you simply should belief your intuition. It's because you do not know which agent is nice and which agent will not be. Carry out research on several brokers by looking out the internet. As soon as if you end up positive that a selected agent is dependable and reliable, you can choose to utilize his partnerise in finding you a home in Singapore. Most of the time, a property agent is taken into account to be good if he or she locations the contact data on his website. This may mean that the agent does not mind you calling them and asking them any questions relating to new properties in singapore in Singapore. After chatting with them you too can see them in their office after taking an appointment.
Have handed an trade examination i.e Widespread Examination for House Brokers (CEHA) or Actual Property Agency (REA) examination, or equal; Exclusive brokers are extra keen to share listing information thus making certain the widest doable coverage inside the real estate community via Multiple Listings and Networking. Accepting a severe provide is simpler since your agent is totally conscious of all advertising activity related with your property. This reduces your having to check with a number of agents for some other offers. Price control is easily achieved. Paint work in good restore-discuss with your Property Marketing consultant if main works are still to be done. Softening in residential property prices proceed, led by 2.8 per cent decline within the index for Remainder of Central Region
Once you place down the one per cent choice price to carry down a non-public property, it's important to accept its situation as it is whenever you move in – faulty air-con, choked rest room and all. Get round this by asking your agent to incorporate a ultimate inspection clause within the possibility-to-buy letter. HDB flat patrons routinely take pleasure in this security net. "There's a ultimate inspection of the property two days before the completion of all HDB transactions. If the air-con is defective, you can request the seller to repair it," says Kelvin.
15.6.1 As the agent is an intermediary, generally, as soon as the principal and third party are introduced right into a contractual relationship, the agent drops out of the image, subject to any problems with remuneration or indemnification that he could have against the principal, and extra exceptionally, against the third occasion. Generally, agents are entitled to be indemnified for all liabilities reasonably incurred within the execution of the brokers´ authority.
To achieve the very best outcomes, you must be always updated on market situations, including past transaction information and reliable projections. You could review and examine comparable homes that are currently available in the market, especially these which have been sold or not bought up to now six months. You'll be able to see a pattern of such report by clicking here It's essential to defend yourself in opposition to unscrupulous patrons. They are often very skilled in using highly unethical and manipulative techniques to try and lure you into a lure. That you must also protect your self, your loved ones, and personal belongings as you'll be serving many strangers in your home. Sign a listing itemizing of all of the objects provided by the proprietor, together with their situation. HSR Prime Recruiter 2010.: translated from the German by Phyllis Fox. This is an earlier version of the paper Template:Harvnb, circulated as a research report. - Many property agents need to declare for the PIC grant in Singapore. However, not all of them know find out how to do the correct process for getting this PIC scheme from the IRAS. There are a number of steps that you need to do before your software can be approved.
Naturally, you will have to pay a safety deposit and that is usually one month rent for annually of the settlement. That is the place your good religion deposit will likely be taken into account and will kind part or all of your security deposit. Anticipate to have a proportionate amount deducted out of your deposit if something is discovered to be damaged if you move out. It's best to you'll want to test the inventory drawn up by the owner, which can detail all objects in the property and their condition. If you happen to fail to notice any harm not already mentioned within the inventory before transferring in, you danger having to pay for it yourself.
In case you are in search of an actual estate or Singapore property agent on-line, you simply should belief your intuition. It's because you do not know which agent is nice and which agent will not be. Carry out research on several brokers by looking out the internet. As soon as if you end up positive that a selected agent is dependable and reliable, you can choose to utilize his partnerise in finding you a home in Singapore. Most of the time, a property agent is taken into account to be good if he or she locations the contact data on his website. This may mean that the agent does not mind you calling them and asking them any questions relating to new properties in singapore in Singapore. After chatting with them you too can see them in their office after taking an appointment.
Have handed an trade examination i.e Widespread Examination for House Brokers (CEHA) or Actual Property Agency (REA) examination, or equal; Exclusive brokers are extra keen to share listing information thus making certain the widest doable coverage inside the real estate community via Multiple Listings and Networking. Accepting a severe provide is simpler since your agent is totally conscious of all advertising activity related with your property. This reduces your having to check with a number of agents for some other offers. Price control is easily achieved. Paint work in good restore-discuss with your Property Marketing consultant if main works are still to be done. Softening in residential property prices proceed, led by 2.8 per cent decline within the index for Remainder of Central Region
Once you place down the one per cent choice price to carry down a non-public property, it's important to accept its situation as it is whenever you move in – faulty air-con, choked rest room and all. Get round this by asking your agent to incorporate a ultimate inspection clause within the possibility-to-buy letter. HDB flat patrons routinely take pleasure in this security net. "There's a ultimate inspection of the property two days before the completion of all HDB transactions. If the air-con is defective, you can request the seller to repair it," says Kelvin.
15.6.1 As the agent is an intermediary, generally, as soon as the principal and third party are introduced right into a contractual relationship, the agent drops out of the image, subject to any problems with remuneration or indemnification that he could have against the principal, and extra exceptionally, against the third occasion. Generally, agents are entitled to be indemnified for all liabilities reasonably incurred within the execution of the brokers´ authority.
To achieve the very best outcomes, you must be always updated on market situations, including past transaction information and reliable projections. You could review and examine comparable homes that are currently available in the market, especially these which have been sold or not bought up to now six months. You'll be able to see a pattern of such report by clicking here It's essential to defend yourself in opposition to unscrupulous patrons. They are often very skilled in using highly unethical and manipulative techniques to try and lure you into a lure. That you must also protect your self, your loved ones, and personal belongings as you'll be serving many strangers in your home. Sign a listing itemizing of all of the objects provided by the proprietor, together with their situation. HSR Prime Recruiter 2010. A freely downlodable copy can be found here.
External links
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- ↑ In general, it is not a sufficient condition; also, it can be a demanding condition for some problems. See the "Implications of the CFL condition" section of this article for a brief survey of these issues.
- ↑ See reference Template:Harvnb. There exists also an English translation of the 1928 German original: see references Template:Harvnb and Template:Harvnb.
- ↑ This situation commonly occurs when a hyperbolic partial differential operator has been approximated by a finite difference equation, which is then solved by numerical linear algebra methods.
- ↑ This quantity is not necessarily the same for each spatial variable, as it is shown in the "The two and general n–dimensional case" section of this entry : it can be chosen in order to somewhat relax the condition.
- ↑ Precisely, this is the hyperbolic part of the PDE under analysis.