This document provides a full numerical solution to the incompressible Couette flow problem using the Crank-Nicolson implicit finite difference method. The Navier-Stokes equations are simplified for this problem and non-dimensionalized. A tridiagonal matrix equation is derived and solved using both the Gauss method and Thomas algorithm. Results show the numerical solution converging to the known analytical solution and demonstrate the effects of varying time step, Reynolds number, and grid density on the velocity field.
FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...ieijjournal
In this paper, we study the numerical solution of singularly perturbed parabolic convection-diffusion type
with boundary layers at the right side. To solve this problem, the backward-Euler with Richardson
extrapolation method is applied on the time direction and the fitted operator finite difference method on the
spatial direction is used, on the uniform grids. The stability and consistency of the method were established
very well to guarantee the convergence of the method. Numerical experimentation is carried out on model
examples, and the results are presented both in tables and graphs. Further, the present method gives a more
accurate solution than some existing methods reported in the literature.
In mathematics, the Lambert W function, also called the omega function or product logarithm, is a set of functions, namely the branches of the inverse relation of the function f(z) = zez where ez is the exponential function and z is any complex number. In other words
{\displaystyle z=f^{-1}(ze^{z})=W(ze^{z})} z=f^{-1}(ze^{z})=W(ze^{z})
By substituting {\displaystyle z'=ze^{z}} z'=ze^{z} in the above equation, we get the defining equation for the W function (and for the W relation in general):
{\displaystyle z'=W(z')e^{W(z')}} z'=W(z')e^{W(z')}
for any complex number z'.
Since the function ƒ is not injective, the relation W is multivalued (except at 0). If we restrict attention to real-valued W, the complex variable z is then replaced by the real variable x, and the relation is defined only for x ≥ −1/e, and is double-valued on (−1/e, 0). The additional constraint W ≥ −1 defines a single-valued function W0(x). We have W0(0) = 0 and W0(−1/e) = −1. Meanwhile, the lower branch has W ≤ −1 and is denoted W−1(x). It decreases from W−1(−1/e) = −1 to W−1(0−) = −∞.
The Lambert W relation cannot be expressed in terms of elementary functions.[1] It is useful in combinatorics, for instance in the enumeration of trees. It can be used to solve various equations involving exponentials (e.g. the maxima of the Planck, Bose–Einstein, and Fermi–Dirac distributions) and also occurs in the solution of delay differential equations, such as y'(t) = a y(t − 1). In biochemistry, and in particular enzyme kinetics, a closed-form solution for the time course kinetics analysis of Michaelis–Menten kinetics is described in terms of the Lambert W function.
The Euler-Mascheroni constant is calculated by three novel representations over these sets respectively: 1) Turán moments, 2) coefficients of Jensen polynomials for the Taylor series of the Riemann Xi function at s = 1/2 + i.t and 3) even coefficients of the Riemann Xi function around s = 1/2.
Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...IOSR Journals
In this paper, a numerical method for Nth - order fuzzy initial value problems (FIVP) based on
Seikkala derivative of fuzzy process is studied. The fourth order Runge-Kutta method based on Centroidal Mean
(RKCeM4) is used to find the numerical solution and the convergence and stability of the method is proved. This
method is illustrated by solving second and third order FIVPs. The results show that the proposed method suits
well to find the numerical solution of Nth – order FIVPs.
FITTED OPERATOR FINITE DIFFERENCE METHOD FOR SINGULARLY PERTURBED PARABOLIC C...ieijjournal
In this paper, we study the numerical solution of singularly perturbed parabolic convection-diffusion type
with boundary layers at the right side. To solve this problem, the backward-Euler with Richardson
extrapolation method is applied on the time direction and the fitted operator finite difference method on the
spatial direction is used, on the uniform grids. The stability and consistency of the method were established
very well to guarantee the convergence of the method. Numerical experimentation is carried out on model
examples, and the results are presented both in tables and graphs. Further, the present method gives a more
accurate solution than some existing methods reported in the literature.
In mathematics, the Lambert W function, also called the omega function or product logarithm, is a set of functions, namely the branches of the inverse relation of the function f(z) = zez where ez is the exponential function and z is any complex number. In other words
{\displaystyle z=f^{-1}(ze^{z})=W(ze^{z})} z=f^{-1}(ze^{z})=W(ze^{z})
By substituting {\displaystyle z'=ze^{z}} z'=ze^{z} in the above equation, we get the defining equation for the W function (and for the W relation in general):
{\displaystyle z'=W(z')e^{W(z')}} z'=W(z')e^{W(z')}
for any complex number z'.
Since the function ƒ is not injective, the relation W is multivalued (except at 0). If we restrict attention to real-valued W, the complex variable z is then replaced by the real variable x, and the relation is defined only for x ≥ −1/e, and is double-valued on (−1/e, 0). The additional constraint W ≥ −1 defines a single-valued function W0(x). We have W0(0) = 0 and W0(−1/e) = −1. Meanwhile, the lower branch has W ≤ −1 and is denoted W−1(x). It decreases from W−1(−1/e) = −1 to W−1(0−) = −∞.
The Lambert W relation cannot be expressed in terms of elementary functions.[1] It is useful in combinatorics, for instance in the enumeration of trees. It can be used to solve various equations involving exponentials (e.g. the maxima of the Planck, Bose–Einstein, and Fermi–Dirac distributions) and also occurs in the solution of delay differential equations, such as y'(t) = a y(t − 1). In biochemistry, and in particular enzyme kinetics, a closed-form solution for the time course kinetics analysis of Michaelis–Menten kinetics is described in terms of the Lambert W function.
The Euler-Mascheroni constant is calculated by three novel representations over these sets respectively: 1) Turán moments, 2) coefficients of Jensen polynomials for the Taylor series of the Riemann Xi function at s = 1/2 + i.t and 3) even coefficients of the Riemann Xi function around s = 1/2.
Numerical Solution of Nth - Order Fuzzy Initial Value Problems by Fourth Orde...IOSR Journals
In this paper, a numerical method for Nth - order fuzzy initial value problems (FIVP) based on
Seikkala derivative of fuzzy process is studied. The fourth order Runge-Kutta method based on Centroidal Mean
(RKCeM4) is used to find the numerical solution and the convergence and stability of the method is proved. This
method is illustrated by solving second and third order FIVPs. The results show that the proposed method suits
well to find the numerical solution of Nth – order FIVPs.
A Proof of Hypothesis Riemann and it is proven that apply only for equation ζ(z)=0.Also here it turns out that it does not apply in General Case.(DOI:10.13140/RG.2.2.10888.34563/5)
constant strain triangular which is used in analysis of triangular in finite element method with the help of shape function and natural coordinate system.
Abstract: The Riemann zeta function is one of the most Leonhard Euler important and fascinating functions in mathematics. Analyzing the matter of conjecture of Riemann divide our analysis in the zeta function and in the proof of conjecture, which has consequences on the distribution of prime numbers.
I am Anthony F. I am a Digital Signal Processing Assignment Expert at matlabassignmentexperts.com. I hold a Ph.D. in Matlab, University of Cambridge, UK. I have been helping students with their homework for the past 8 years. I solve assignments related to Digital Signal Processing.
Visit matlabassignmentexperts.com or email info@matlabassignmentexperts.com.
You can also call on +1 678 648 4277 for any assistance with Digital Signal Processing Assignments.
It turns out that an equation x^p+y^q=z^w has a solution in Z+ if and only if at least one exponent p or q or w equals 2.DOI:10.13140/RG.2.2.15459.22567/7
Lesson 19: The Mean Value Theorem (Section 041 handout)Matthew Leingang
The Mean Value Theorem is the most important theorem in calculus. It is the first theorem which allows us to infer information about a function from information about its derivative. From the MVT we can derive tests for the monotonicity (increase or decrease) and concavity of a function.
A Proof of Hypothesis Riemann and it is proven that apply only for equation ζ(z)=0.Also here it turns out that it does not apply in General Case.(DOI:10.13140/RG.2.2.10888.34563/5)
constant strain triangular which is used in analysis of triangular in finite element method with the help of shape function and natural coordinate system.
Abstract: The Riemann zeta function is one of the most Leonhard Euler important and fascinating functions in mathematics. Analyzing the matter of conjecture of Riemann divide our analysis in the zeta function and in the proof of conjecture, which has consequences on the distribution of prime numbers.
I am Anthony F. I am a Digital Signal Processing Assignment Expert at matlabassignmentexperts.com. I hold a Ph.D. in Matlab, University of Cambridge, UK. I have been helping students with their homework for the past 8 years. I solve assignments related to Digital Signal Processing.
Visit matlabassignmentexperts.com or email info@matlabassignmentexperts.com.
You can also call on +1 678 648 4277 for any assistance with Digital Signal Processing Assignments.
It turns out that an equation x^p+y^q=z^w has a solution in Z+ if and only if at least one exponent p or q or w equals 2.DOI:10.13140/RG.2.2.15459.22567/7
Lesson 19: The Mean Value Theorem (Section 041 handout)Matthew Leingang
The Mean Value Theorem is the most important theorem in calculus. It is the first theorem which allows us to infer information about a function from information about its derivative. From the MVT we can derive tests for the monotonicity (increase or decrease) and concavity of a function.
SUCCESSIVE LINEARIZATION SOLUTION OF A BOUNDARY LAYER CONVECTIVE HEAT TRANSFE...ijcsa
The purpose of this paper is to discuss the flow of forced convection over a flat plate. The governing partial
differential equations are transformed into ordinary differential equations using suitable transformations.
The resulting equations were solved using a recent semi-numerical scheme known as the successive
linearization method (SLM). A comparison between the obtained results with homotopy perturbation method and numerical method (NM) has been included to test the accuracy and convergence of the method.
Numerical Methods in Mechanical Engineering - Final ProjectStasik Nemirovsky
Final Project for the class of "Numerical Methods in Mechanical Engineering" - MECH 309.
In this project, various engineering problems were analyzed and solved using advanced numerical approximation methods and MATLAB software.
All of material inside is un-licence, kindly use it for educational only but please do not to commercialize it.
Based on 'ilman nafi'an, hopefully this file beneficially for you.
Thank you.
My paper for Domain Decomposition Conference in Strobl, Austria, 2005Alexander Litvinenko
We did a first step in solving, so-called, skin problem. We developed an efficient H-matrix preconditioner to solve diffusion problem with jumping coefficients
In the vast landscape of cinema, stories have been told, retold, and reimagined in countless ways. At the heart of this narrative evolution lies the concept of a "remake". A successful remake allows us to revisit cherished tales through a fresh lens, often reflecting a different era's perspective or harnessing the power of advanced technology. Yet, the question remains, what makes a remake successful? Today, we will delve deeper into this subject, identifying the key ingredients that contribute to the success of a remake.
Skeem Saam in June 2024 available on ForumIsaac More
Monday, June 3, 2024 - Episode 241: Sergeant Rathebe nabs a top scammer in Turfloop. Meikie is furious at her uncle's reaction to the truth about Ntswaki.
Tuesday, June 4, 2024 - Episode 242: Babeile uncovers the truth behind Rathebe’s latest actions. Leeto's announcement shocks his employees, and Ntswaki’s ordeal haunts her family.
Wednesday, June 5, 2024 - Episode 243: Rathebe blocks Babeile from investigating further. Melita warns Eunice to stay clear of Mr. Kgomo.
Thursday, June 6, 2024 - Episode 244: Tbose surrenders to the police while an intruder meddles in his affairs. Rathebe's secret mission faces a setback.
Friday, June 7, 2024 - Episode 245: Rathebe’s antics reach Kganyago. Tbose dodges a bullet, but a nightmare looms. Mr. Kgomo accuses Melita of witchcraft.
Monday, June 10, 2024 - Episode 246: Ntswaki struggles on her first day back at school. Babeile is stunned by Rathebe’s romance with Bullet Mabuza.
Tuesday, June 11, 2024 - Episode 247: An unexpected turn halts Rathebe’s investigation. The press discovers Mr. Kgomo’s affair with a young employee.
Wednesday, June 12, 2024 - Episode 248: Rathebe chases a criminal, resorting to gunfire. Turf High is rife with tension and transfer threats.
Thursday, June 13, 2024 - Episode 249: Rathebe traps Kganyago. John warns Toby to stop harassing Ntswaki.
Friday, June 14, 2024 - Episode 250: Babeile is cleared to investigate Rathebe. Melita gains Mr. Kgomo’s trust, and Jacobeth devises a financial solution.
Monday, June 17, 2024 - Episode 251: Rathebe feels the pressure as Babeile closes in. Mr. Kgomo and Eunice clash. Jacobeth risks her safety in pursuit of Kganyago.
Tuesday, June 18, 2024 - Episode 252: Bullet Mabuza retaliates against Jacobeth. Pitsi inadvertently reveals his parents’ plans. Nkosi is shocked by Khwezi’s decision on LJ’s future.
Wednesday, June 19, 2024 - Episode 253: Jacobeth is ensnared in deceit. Evelyn is stressed over Toby’s case, and Letetswe reveals shocking academic results.
Thursday, June 20, 2024 - Episode 254: Elizabeth learns Jacobeth is in Mpumalanga. Kganyago's past is exposed, and Lehasa discovers his son is in KZN.
Friday, June 21, 2024 - Episode 255: Elizabeth confirms Jacobeth’s dubious activities in Mpumalanga. Rathebe lies about her relationship with Bullet, and Jacobeth faces theft accusations.
Monday, June 24, 2024 - Episode 256: Rathebe spies on Kganyago. Lehasa plans to retrieve his son from KZN, fearing what awaits.
Tuesday, June 25, 2024 - Episode 257: MaNtuli fears for Kwaito’s safety in Mpumalanga. Mr. Kgomo and Melita reconcile.
Wednesday, June 26, 2024 - Episode 258: Kganyago makes a bold escape. Elizabeth receives a shocking message from Kwaito. Mrs. Khoza defends her husband against scam accusations.
Thursday, June 27, 2024 - Episode 259: Babeile's skillful arrest changes the game. Tbose and Kwaito face a hostage crisis.
Friday, June 28, 2024 - Episode 260: Two women face the reality of being scammed. Turf is rocked by breaking
Panchayat Season 3 - Official Trailer.pdfSuleman Rana
The dearest series "Panchayat" is set to make a victorious return with its third season, and the fervor is discernible. The authority trailer, delivered on May 28, guarantees one more enamoring venture through the country heartland of India.
Jitendra Kumar keeps on sparkling as Abhishek Tripathi, the city-reared engineer who ends up functioning as the secretary of the Panchayat office in the curious town of Phulera. His nuanced depiction of a young fellow exploring the difficulties of country life while endeavoring to adjust to his new environmental factors has earned far and wide recognition.
Neena Gupta and Raghubir Yadav return as Manju Devi and Brij Bhushan Dubey, separately. Their dynamic science and immaculate acting rejuvenate the hardships of town administration. Gupta's depiction of the town Pradhan with an ever-evolving outlook, matched with Yadav's carefully prepared exhibition, adds profundity and credibility to the story.
New Difficulties and Experiences
The trailer indicates new difficulties anticipating the characters, as Abhishek keeps on wrestling with his part in the town and his yearnings for a superior future. The series has reliably offset humor with social editorial, and Season 3 looks ready to dig much more profound into the intricacies of rustic organization and self-awareness.
Watchers can hope to see a greater amount of the enchanting and particular residents who have become fan top picks. Their connections and the one of a kind cut of-life situations give a reviving and interesting portrayal of provincial India, featuring the two its appeal and its difficulties.
A Mix of Humor and Heart
One of the signs of "Panchayat" is its capacity to mix humor with sincere narrating. The trailer features minutes that guarantee to convey giggles, as well as scenes that pull at the heartstrings. This equilibrium has been a critical calculate the show's prosperity, resounding with crowds across different socioeconomics.
Creation Greatness
The creation quality remaining parts first rate, with the beautiful setting of Phulera town filling in as a scenery that upgrades the narrating. The meticulousness in portraying provincial life, joined with sharp composition and solid exhibitions, guarantees that "Panchayat" keeps on hanging out in the packed web series scene.
Expectation and Delivery
As the delivery date draws near, expectation for "Panchayat" Season 3 is at a record-breaking high. The authority trailer has previously created critical buzz, with fans enthusiastically anticipating the continuation of Abhishek Tripathi's excursion and the new undertakings that lie ahead in Phulera.
All in all, the authority trailer for "Panchayat" Season 3 recommends that watchers are in for another drawing in and engaging ride. Yet again with its charming characters, convincing story, and ideal mix of humor and show, the new season is set to enamor crowds. Write in your schedules and prepare to get back to the endearing universe of "Panchayat."
Meet Crazyjamjam - A TikTok Sensation | Blog EternalBlog Eternal
Crazyjamjam, the TikTok star everyone's talking about! Uncover her secrets to success, viral trends, and more in this exclusive feature on Blog Eternal.
Source: https://blogeternal.com/celebrity/crazyjamjam-leaks/
Young Tom Selleck: A Journey Through His Early Years and Rise to Stardomgreendigital
Introduction
When one thinks of Hollywood legends, Tom Selleck is a name that comes to mind. Known for his charming smile, rugged good looks. and the iconic mustache that has become synonymous with his persona. Tom Selleck has had a prolific career spanning decades. But, the journey of young Tom Selleck, from his early years to becoming a household name. is a story filled with determination, talent, and a touch of luck. This article delves into young Tom Selleck's life, background, early struggles. and pivotal moments that led to his rise in Hollywood.
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Early Life and Background
Family Roots and Childhood
Thomas William Selleck was born in Detroit, Michigan, on January 29, 1945. He was the second of four children in a close-knit family. His father, Robert Dean Selleck, was a real estate investor and executive. while his mother, Martha Selleck, was a homemaker. The Selleck family relocated to Sherman Oaks, California. when Tom was a child, setting the stage for his future in the entertainment industry.
Education and Early Interests
Growing up, young Tom Selleck was an active and athletic child. He attended Grant High School in Van Nuys, California. where he excelled in sports, particularly basketball. His tall and athletic build made him a standout player, and he earned a basketball scholarship to the University of Southern California (U.S.C.). While at U.S.C., Selleck studied business administration. but his interests shifted toward acting.
Discovery of Acting Passion
Tom Selleck's journey into acting was serendipitous. During his time at U.S.C., a drama coach encouraged him to try acting. This nudge led him to join the Hills Playhouse, where he began honing his craft. Transitioning from an aspiring athlete to an actor took time. but young Tom Selleck became drawn to the performance world.
Early Career Struggles
Breaking Into the Industry
The path to stardom was a challenging one for young Tom Selleck. Like many aspiring actors, he faced many rejections and struggled to find steady work. A series of minor roles and guest appearances on television shows marked his early career. In 1965, he debuted on the syndicated show "The Dating Game." which gave him some exposure but did not lead to immediate success.
The Commercial Breakthrough
During the late 1960s and early 1970s, Selleck began appearing in television commercials. His rugged good looks and charismatic presence made him a popular brand choice. He starred in advertisements for Pepsi-Cola, Revlon, and Close-Up toothpaste. These commercials provided financial stability and helped him gain visibility in the industry.
Struggling Actor in Hollywood
Despite his success in commercials. breaking into large acting roles remained a challenge for young Tom Selleck. He auditioned and took on small parts in T.V. shows and movies. Some of his early television appearances included roles in popular series like Lancer, The F.B.I., and Bracken's World. But, it would take a
Maximizing Your Streaming Experience with XCIPTV- Tips for 2024.pdfXtreame HDTV
In today’s digital age, streaming services have become an integral part of our entertainment lives. Among the myriad of options available, XCIPTV stands out as a premier choice for those seeking seamless, high-quality streaming. This comprehensive guide will delve into the features, benefits, and user experience of XCIPTV, illustrating why it is a top contender in the IPTV industry.
Meet Dinah Mattingly – Larry Bird’s Partner in Life and Loveget joys
Get an intimate look at Dinah Mattingly’s life alongside NBA icon Larry Bird. From their humble beginnings to their life today, discover the love and partnership that have defined their relationship.
From Slave to Scourge: The Existential Choice of Django Unchained. The Philos...Rodney Thomas Jr
#SSAPhilosophy #DjangoUnchained #DjangoFreeman #ExistentialPhilosophy #Freedom #Identity #Justice #Courage #Rebellion #Transformation
Welcome to SSA Philosophy, your ultimate destination for diving deep into the profound philosophies of iconic characters from video games, movies, and TV shows. In this episode, we explore the powerful journey and existential philosophy of Django Freeman from Quentin Tarantino’s masterful film, "Django Unchained," in our video titled, "From Slave to Scourge: The Existential Choice of Django Unchained. The Philosophy of Django Freeman!"
From Slave to Scourge: The Existential Choice of Django Unchained – The Philosophy of Django Freeman!
Join me as we delve into the existential philosophy of Django Freeman, uncovering the profound lessons and timeless wisdom his character offers. Through his story, we find inspiration in the power of choice, the quest for justice, and the courage to defy oppression. Django Freeman’s philosophy is a testament to the human spirit’s unyielding drive for freedom and justice.
Don’t forget to like, comment, and subscribe to SSA Philosophy for more in-depth explorations of the philosophies behind your favorite characters. Hit the notification bell to stay updated on our latest videos. Let’s discover the principles that shape these icons and the profound lessons they offer.
Django Freeman’s story is one of the most compelling narratives of transformation and empowerment in cinema. A former slave turned relentless bounty hunter, Django’s journey is not just a physical liberation but an existential quest for identity, justice, and retribution. This video delves into the core philosophical elements that define Django’s character and the profound choices he makes throughout his journey.
Link to video: https://youtu.be/GszqrXk38qk
Scandal! Teasers June 2024 on etv Forum.co.zaIsaac More
Monday, 3 June 2024
Episode 47
A friend is compelled to expose a manipulative scheme to prevent another from making a grave mistake. In a frantic bid to save Jojo, Phakamile agrees to a meeting that unbeknownst to her, will seal her fate.
Tuesday, 4 June 2024
Episode 48
A mother, with her son's best interests at heart, finds him unready to heed her advice. Motshabi finds herself in an unmanageable situation, sinking fast like in quicksand.
Wednesday, 5 June 2024
Episode 49
A woman fabricates a diabolical lie to cover up an indiscretion. Overwhelmed by guilt, she makes a spontaneous confession that could be devastating to another heart.
Thursday, 6 June 2024
Episode 50
Linda unwittingly discloses damning information. Nhlamulo and Vuvu try to guide their friend towards the right decision.
Friday, 7 June 2024
Episode 51
Jojo's life continues to spiral out of control. Dintle weaves a web of lies to conceal that she is not as successful as everyone believes.
Monday, 10 June 2024
Episode 52
A heated confrontation between lovers leads to a devastating admission of guilt. Dintle's desperation takes a new turn, leaving her with dwindling options.
Tuesday, 11 June 2024
Episode 53
Unable to resort to violence, Taps issues a verbal threat, leaving Mdala unsettled. A sister must explain her life choices to regain her brother's trust.
Wednesday, 12 June 2024
Episode 54
Winnie makes a very troubling discovery. Taps follows through on his threat, leaving a woman reeling. Layla, oblivious to the truth, offers an incentive.
Thursday, 13 June 2024
Episode 55
A nosy relative arrives just in time to thwart a man's fatal decision. Dintle manipulates Khanyi to tug at Mo's heartstrings and get what she wants.
Friday, 14 June 2024
Episode 56
Tlhogi is shocked by Mdala's reaction following the revelation of their indiscretion. Jojo is in disbelief when the punishment for his crime is revealed.
Monday, 17 June 2024
Episode 57
A woman reprimands another to stay in her lane, leading to a damning revelation. A man decides to leave his broken life behind.
Tuesday, 18 June 2024
Episode 58
Nhlamulo learns that due to his actions, his worst fears have come true. Caiphus' extravagant promises to suppliers get him into trouble with Ndu.
Wednesday, 19 June 2024
Episode 59
A woman manages to kill two birds with one stone. Business doom looms over Chillax. A sobering incident makes a woman realize how far she's fallen.
Thursday, 20 June 2024
Episode 60
Taps' offer to help Nhlamulo comes with hidden motives. Caiphus' new ideas for Chillax have MaHilda excited. A blast from the past recognizes Dintle, not for her newfound fame.
Friday, 21 June 2024
Episode 61
Taps is hungry for revenge and finds a rope to hang Mdala with. Chillax's new job opportunity elicits mixed reactions from the public. Roommates' initial meeting starts off on the wrong foot.
Monday, 24 June 2024
Episode 62
Taps seizes new information and recruits someone on the inside. Mary's new job
As a film director, I have always been awestruck by the magic of animation. Animation, a medium once considered solely for the amusement of children, has undergone a significant transformation over the years. Its evolution from a rudimentary form of entertainment to a sophisticated form of storytelling has stirred my creativity and expanded my vision, offering limitless possibilities in the realm of cinematic storytelling.
240529_Teleprotection Global Market Report 2024.pdfMadhura TBRC
The teleprotection market size has grown
exponentially in recent years. It will grow from
$21.92 billion in 2023 to $28.11 billion in 2024 at a
compound annual growth rate (CAGR) of 28.2%. The
teleprotection market size is expected to see
exponential growth in the next few years. It will grow
to $70.77 billion in 2028 at a compound annual
growth rate (CAGR) of 26.0%.
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Tom Selleck Net Worth: A Comprehensive Analysisgreendigital
Over several decades, Tom Selleck, a name synonymous with charisma. From his iconic role as Thomas Magnum in the television series "Magnum, P.I." to his enduring presence in "Blue Bloods," Selleck has captivated audiences with his versatility and charm. As a result, "Tom Selleck net worth" has become a topic of great interest among fans. and financial enthusiasts alike. This article delves deep into Tom Selleck's wealth, exploring his career, assets, endorsements. and business ventures that contribute to his impressive economic standing.
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Early Life and Career Beginnings
The Foundation of Tom Selleck's Wealth
Born on January 29, 1945, in Detroit, Michigan, Tom Selleck grew up in Sherman Oaks, California. His journey towards building a large net worth began with humble origins. , Selleck pursued a business administration degree at the University of Southern California (USC) on a basketball scholarship. But, his interest shifted towards acting. leading him to study at the Hills Playhouse under Milton Katselas.
Minor roles in television and films marked Selleck's early career. He appeared in commercials and took on small parts in T.V. series such as "The Dating Game" and "Lancer." These initial steps, although modest. laid the groundwork for his future success and the growth of Tom Selleck net worth. Breakthrough with "Magnum, P.I."
The Role that Defined Tom Selleck's Career
Tom Selleck's breakthrough came with the role of Thomas Magnum in the CBS television series "Magnum, P.I." (1980-1988). This role made him a household name and boosted his net worth. The series' popularity resulted in Selleck earning large salaries. leading to financial stability and increased recognition in Hollywood.
"Magnum P.I." garnered high ratings and critical acclaim during its run. Selleck's portrayal of the charming and resourceful private investigator resonated with audiences. making him one of the most beloved television actors of the 1980s. The success of "Magnum P.I." played a pivotal role in shaping Tom Selleck net worth, establishing him as a major star.
Film Career and Diversification
Expanding Tom Selleck's Financial Portfolio
While "Magnum, P.I." was a cornerstone of Selleck's career, he did not limit himself to television. He ventured into films, further enhancing Tom Selleck net worth. His filmography includes notable movies such as "Three Men and a Baby" (1987). which became the highest-grossing film of the year, and its sequel, "Three Men and a Little Lady" (1990). These box office successes contributed to his wealth.
Selleck's versatility allowed him to transition between genres. from comedies like "Mr. Baseball" (1992) to westerns such as "Quigley Down Under" (1990). This diversification showcased his acting range. and provided many income streams, reinforcing Tom Selleck net worth.
Television Resurgence with "Blue Bloods"
Sustaining Wealth through Consistent Success
In 2010, Tom Selleck began starring as Frank Reagan i
Create a Seamless Viewing Experience with Your Own Custom OTT Player.pdfGenny Knight
As the popularity of online streaming continues to rise, the significance of providing outstanding viewing experiences cannot be emphasized enough. Tailored OTT players present a robust solution for service providers aiming to enhance their offerings and engage audiences in a competitive market. Through embracing customization, companies can craft immersive, individualized experiences that effectively hold viewers' attention, entertain them, and encourage repeat usage.
Experience the thrill of Progressive Puzzle Adventures, like Scavenger Hunt Games and Escape Room Activities combined Solve Treasure Hunt Puzzles online.
From the Editor's Desk: 115th Father's day Celebration - When we see Father's day in Hindu context, Nanda Baba is the most vivid figure which comes to the mind. Nanda Baba who was the foster father of Lord Krishna is known to provide love, care and affection to Lord Krishna and Balarama along with his wife Yashoda; Letter’s to the Editor: Mother's Day - Mother is a precious life for their children. Mother is life breath for her children. Mother's lap is the world happiness whose debt can never be paid.
1. arXiv:physics/0302010v1[physics.comp-ph]4Feb2003
Incompressible Couette Flow ∗
Maciej Matyka†
email: maq@panoramix.ift.uni.wroc.pl
Exchange Student
at
University of Linkoping
Abstract
This project work report provides a full solution of
simplified Navier Stokes equations for The Incom-
pressible Couette Problem. The well known analyt-
ical solution to the problem of incompressible cou-
ette is compared with a numerical solution. In that
paper, I will provide a full solution with simple C
code instead of MatLab or Fortran codes, which are
known. For discrete problem formulation, implicit
Crank-Nicolson method was used. Finally, the sys-
tem of equation (tridiagonal) is solved with both
Thomas and simple Gauss Method. Results of both
methods are compared.
1 Introduction
Main problem is shown in figure (1). There is
viscous flow between two parallel plates. Upper
plate is moving in x direction with constans velocity
(U = Ue). Lower one is not moving (U = 0). We
are looking for a solution to describe velocity vector
field in the model (between two plates).
∗Thanks for Grzegorz Juraszek (for English languague
checking).
†Student of Computational Physics subsection of Theo-
retical Physics at University of Wroclaw in Poland. Depar-
tament of Physics and Astronomy.
U=Ue
U=0
D Flow
Figure 1: Schematic representation of Couette Flow
Problem
2 Fundamental Equations
Most of incompressible fluid mechanics (dynam-
ics) problems are described by simple Navier-Stokes
equation for incompressible fluid velocity, which can
be written with a form:
∂u
∂t
= (−u∇)u − ∇ϕ + υ∇2
u + g, (1)
where ϕ is defined is defined as the relation of
pressure to density:
ϕ =
p
ρ
(2)
and υ is a kinematics viscosity of the fluid.
We will also use a continuity equation, which can
be written as follows 1
:
1I assume constans density of the fluid.
2. D = ∇ · v = 0 (3)
Of course, in a case of couette incompressible flow
we will use several simplifications of (1).
3 Mathematical Formulation
of the Couette Problem
Incompressible couette problem is not needed to
solve full Navier-Stokes equations. There is no ex-
ternal force, so first simplification of (1) will be:
∂u
∂t
= (−u∇)u − ∇ϕ + υ∇2
u, (4)
In [1] there can be found easy proof that in cou-
ette problem there are no pressure gradients, which
means that:
∇ϕ = 0, (5)
We will ignore a convection effects so, equation
(4) can be written with a form:
∂u
∂t
= υ∇2
u (6)
Now we have simple differential equation for ve-
locity vector field. That equation is a vector type
and can be simplified even more. Let us write
continuity equation (3) in differential form. Let
u = (u, v), then continuity equation can be ex-
panded as follows2
:
∂u
∂x
+
∂v
∂y
= 0 (7)
We know that there is no u velocity component
gradient along x axis (symmetry of the problem),
so:
∂u
∂x
= 0 (8)
Evaluation of Taylor series3
at points y = 0 and
y = D gives us a proof that only one possible and
physically correct value for y component of velocity
u is:
v = 0 (9)
Because of (9) equation (6) can be written as fol-
lows:
2Only with assumption of non compressible fluid.
3Those simple expressions can be found in [1], chapter
9.2.
∂u
∂t
= υ
∂2
u
∂y2
(10)
Our problem is now simplified to mathematical
problem of solving equations like (10). That is now
a governing problem of incompressible couette flow
analysis.
3.1 Analytical soulution
Analytical solution for velocity profile of steady
flow, without time-changes (steady state) can be
found very easily in an equation:
υ
∂2
u
∂y2
= 0 (11)
And without any changes of viscosity υ it can be
written in form:
∂2
u
∂y2
= 0 (12)
After simple two times integration of equation
(12) we have analytical solution function of (12):
u = c1 · y + c2 (13)
where c1 and c2 are integration constans.
3.2 Boundary Conditions for The
Analytical Solution
Simple boundary conditions are provided in that
problem. We know that:
u =
0 y=0
ue y=D
(14)
Simple applying it to our solution (13) gives a
more specified one, where c1 = ue
D and c2 = 0:
u =
ue
D
· y (15)
It means, that a relationship between u and y is
linear. A Better idea to write that with mathemat-
ical expression is:
u
y
=
ue
D
(16)
Where ue
D is a constans for the problem (initial u
velocity vs size of the model).
2
3. 4 Numerical Solution
4.1 Non-dimensional Form
Let us define some new non-dimensional variables4
:
u =
u
′
= u
ue
y
′
= y
D
t
′
= t
D/ue
(17)
Now let us place these variables into equation
(10) and we have now a non-dimensional equation
written as follows:
ρ
∂u/ue
(t · ue)/D
u2
e
D
= υ
∂2
(u/ue)
∂(y/D)2
ue
D2
(18)
Now we replace all the variables to nondimen-
sional, like defined in (17):
ρ
∂u
′
∂t′
u2
e
D
= υ
∂2
u
′
∂y′2
ue
D2
(19)
Now we will remove all
′
chars from that equa-
tion (only for simplification of notation), and the
equation becomes5
to:
∂u
∂t
=
υ
Dρue
∂2
u
∂y2
(20)
In that equation Reynold’s number Re appears,
and is defined as:
Re =
Dρue
υ
(21)
Where Re is Reynold’s number that depends on
D height of couette model. Finally, the last form of
the equation for the couette problem can be written
as follows:
∂u
∂t
=
1
Re
∂2
u
∂y2
(22)
We will try to formulate numerical solution of the
equation (22).
4.2 Finite - Difference Representa-
tion
In our solution of equation (22) we will use Crank-
Nicolson technique, so discrete representation of
that equation can be written 6
as:
4Exacly the same, like in [1].
5Constans simplification also implemented
6That representation is based on central discrete differen-
tial operators.
un+1
j = un
j +
∆t
2(∆y)2Re
(un+1
j+1 +un
j+1−2un+1
j +un+1
j−1 +un
j−1)
(23)
Simple grouping of all terms which are placed in
time step (n+1) on the left side and rest of them
- on right side, gives us an equation which can be
written as:
Aun+1
j−1 + Bun+1
j + Aun+1
j+1 = Kj (24)
Where Kj is known and depends only on values
u at n time step:
Kj = 1 −
∆t
(∆y)2Re
un
j +
∆t
2(∆y)2Re
(un
j+1 +un
j−1)
(25)
Constans A and B are defined as follows7
:
A = −
∆t
2(∆y)2Re
(26)
B = 1 +
∆t
(∆y)2Re
(27)
4.3 Crank - Nicolson Implicit scheme
For numerical solution we will use one-dimensional
grid points (1, . . . , N + 1) where we will keep cal-
culated u velocities. That means u has values from
the range (u1, u2, . . . , uN+1). We know (from fixed
boundary conditions), that: u1 = 0 and uN+1 = 0.
Simple analysis of the equation (24) gives us a sys-
tem of equations, which can be described by matrix
equation:
A · X = Y (28)
Where A is tridiagonal [N − 1] · [N − 1] matrix
of constant A and B values:
A =
B A
A B A
. . .
. . .
A B A
A B
(29)
X vector is a vector of u values:
X = [u1, u2, . . . , uN+1] (30)
7Directly from equation (23).
3
4. Y vector is a vector of constans Kj values:
Y = [K1, . . . , KN+1] (31)
5 Solving The System of Lin-
ear Equations
Now the problem comes to solving the matrix - vec-
tor equation (28). There are a lot of numerical
methods for that8
, and we will try to choose two
of them: Thomas and Gauss method. Both are
very similar, and I will start with a description of
my implementation with the simple Gauss method.
5.1 Gauss Method
Choice of the Gauss method for solving system of
linear equations is the easiest way. This simple al-
gorithm is well known, and we can do it very easily
by hand on the paper. However, for big matrices
(big N value) a computer program will provide us
with a fast and precise solution. A very important
thing is that time spent on writing (or implement-
ing, if Gauss procedure was written before) is very
short, because of its simplicity.
I used a Gauss procedure with partial choice of
a/the general element. That is a well known tech-
nique for taking the first element from a column of
a matrix for better numerical accuracy.
The whole Gauss procedure of solving a system of
equations contains three steps. First, we are look-
ing for the general element.
After that, when a general element is in the first
row (we make an exchange of rows9
) we make some
simple calculations (for every value in every row
and column of the matrix) for the simplified matrix
to be diagonal (instead of a tridiagonal one which
we have at the beginning). That is all, because af-
ter diagonalization I implement a simple procedure
(from the end row to the start row of the matrix)
which calculates the whole vector X. There are my
values of ui velocity in all the model10
.
5.2 Thomas Method
Thomas’ method, described in [1] is simplified ver-
sion of Gauss method, created especially for tridiag-
8Especially for tridiagonal matrices like A
9We made it for A matrix, and for X, Y too.
10More detailed description of Gauss method can be found
in a lot of books on numerical methods, like [2].
onal matrices. There is one disadvantage of Gauss
method which disappears when Thomas’ method is
implemented. Gauss method is rather slow, and
lot of computational time is lost, because of special
type of matrix. Tridiagonal matrices contain a lot
of free (zero) values. In the Gauss method these
values joins the calculation, what is useless.
Thomas’ simplification for tridiagonal matrices is
to get only values from non-zero tridiagonal part of
matrix. Simply applying a Thomas’ equations for
our governing matrix equation (28) gives us:
d
′
i = B −
A2
d
′
i−1
(32)
u
′
i = ui −
u
′
iA
d
′
i−1
(33)
We know that exact value of uM is defined as
follows:
uM =
u
′
M
B
(34)
Now solution of the system of equations will be
rather easy. We will use recursion like that:
ui−1 =
u
′
i−1 − A · ui
B
(35)
That easy recursion provides us a solution for the
linear system of equations.
6 Results
Main results are provided as plots of the function:
y
D
= f
u
ue
(36)
In figure (2) there is drawn an analytical solu-
tion to the problem of couette flow. That is linear
function, and we expect that after a several time
steps of numerical procedure we will have the same
configuration of velocity field.
6.1 Different Time Steps
In figure (3) there are results of velocity u calcu-
lation for several different time steps. Analytical
solution is also drawn there.
As we can see in the figure (3) - the solution is
going to be same as analytical one. Beginning state
(known from boundary conditions) is changing and
relaxing.
4
5. 0
0.2
0.4
0.6
0.8
1
0 0.2 0.4 0.6 0.8 1
y/D
u/u_e
analitycal solution
Figure 2: Analytical exact solution.
0
0.2
0.4
0.6
0.8
1
0 0.2 0.4 0.6 0.8 1
y/D
u/u_e
step=4
step=8
step=15
step=35
step=69
step=122
analitycal solution
Figure 3: Results for different time steps of numer-
ical calculations.
6.2 Results for Different Reynolds
Numbers
In the figure (4) there is plot of numerical calcula-
tions for different Reynold’s numbers. For example
Reynold’s number depends on i.e. viscosity of the
fluid, size of couette model. As it is shown on the
plot there is strong relationship between the speed
of the velocity field changes and Reynold’s number.
In a couple of words: when Reynolds number in-
creases - frequency of changes also increases.
6.3 Results for Different Grid Den-
sity
In figure (5) there is an example of calculations of
velocity field for different grid density (N number).
0
0.2
0.4
0.6
0.8
1
0 0.2 0.4 0.6 0.8 1
y/D
u/u_e
Re=500
Re=2000
Re=5000
Re=10000
Figure 4: Calculation for same time (t = 2500) and
different Reynold’s numbers.
We see that there is also strong correlation between
grid density, and speed of changes on the grid. Also,
very interesting case N = 10 shows, that for low
density of the grid changes are very fast, and not
accurate.
0
0.2
0.4
0.6
0.8
1
0 0.2 0.4 0.6 0.8 1
y/D
u/u_e
N=10
N=15
N=20
N=30
N=50
Figure 5: Calculation for same time (t = 2500),
same Reynold’s numbers (Re=5000) and different
grid density (N number).
6.4 Conclusion
Solving of Incompressible Couette Problem can be
good way to check numerical method, because of
existing analytical solution. In that report there
were presented two methods of solving system of
equations: Gauss and Thomas’ method. System of
equations was taken from Crank-Nicolson Implicit
5
10. printf(",J,Y[J],U[j]n"); // info 2
for(j=1;j<=NN;j++)
printf("%d , %f, %fn",j,U[j],Y[j]);
printf("n n n n"); // for nice view of several datas
}
}
return (1);
}
8 APPENDIX B
#include <stdlib.h>
#include <stdio.h>
#define N (50)
#define NN (N+1)
int main(void)
{
double U[N*2+2],A[N*2+2],B[N*2+2],C[N*2+2],D[N*2+2],Y[N*2+2];
// initialization
double OneOverN = 1.0/(double)N;
double Re=7000; // Reynolds number
double EE=1.0; // dt parameter
double t=0;
double dt=EE*Re*OneOverN*2; // delta time
double AA=-0.5*EE;
double BB=1.0+EE;
int KKEND=122;
int KKMOD=1;
int KK; // for a loop
int j,k; // for loops too
int M; // temporary needed variable
double test;
Y[1]=0; // init
// apply boundary conditions for Couette Problem
U[1]=0.0;
U[NN]=1.0;
// initial conditions (zero as values of vertical velocity inside of the couette model)
for(j=2;j<=N;j++)
U[j]=0.0;
A[1]=B[1]=C[1]=D[1]=1.0;
printf("dt=%f, Re=%f, N=%d n",dt,Re, N);
10
12. References
[1] John D. Andertson, Jr. ’Computational Fluid Dynamics: The Basics with Applications’, McGraw-
Hill Inc, 1995.
[2] David Potter ’Metody obliczeniowe fizyki’, PWN 1982.
[3] Ryszard Grybos, ’Podstawy mechaniki plynow’ (Tom 1 i 2), PWN 1998.
12