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Cellular automaton A cellular automaton (plural: cellular automata) is a discrete model studied in computability theory, mathematics, theoretical biology and microstructure modeling. It consists of a regular grid of cells, each in one of a finite number of states. The grid can be in any finite number of dimensions. Time is also discrete, and the state of a cell at time t is a function of the states of a finite number of cells (called its neighborhood) at time t ? 1. These neighbors are a selection of cells relative to the specified cell, and do not change (though the cell itself may be in its neighborhood, it is not usually considered a neighbor). Every cell has the same rule for updating, based on the values in this neighbourhood. Each time the rules are applied to the whole grid a new generation is created. One way to simulate a two-dimensional cellular automaton is with an infinite sheet of graph paper along with a set of rules for the cells to follow. Each square is called a "cell" and each cell has two possible states, black and white. The "neighbors" of a cell are the 8 squares touching it. For such a cell and its neighbors, there are 512 (= 29) possible patterns. For each of the 512 possible patterns, the rule table would state whether the center cell will be black or white on the next time interval. Conway"s Game of Life is a popular version of this model. It is usually assumed that every cell in the universe starts in the same state, except for a finite number of cells in other states, often called a configuration. More generally, it is sometimes assumed that the universe starts out covered with a periodic pattern, and only a finite number of cells violate that pattern. The latter assumption is common in one-dimensional cellular automata. Cellular automata are often simulated on a finite grid rather than an infinite one. In two dimensions, the universe would be a rectangle instead of an infinite plane. The obvious problem with finite grids is how to handle the cells on the edges. How they are handled will affect the values of all the cells in the grid. One possible method is to allow the values in those cells to remain constant. Another method is to define neighbourhoods differently for these cells. One could say that they have fewer neighbours, but then one would also have to define new rules for the cells located on the edges. These cells are usually handled with a toroidal arrangement: when one goes off the top, one comes in at the corresponding position on the bottom, and when one goes off the left, one comes in on the right. (This essentially simulates an infinite periodic tiling, and in the field of partial differential equations is sometimes referred to as periodic boundary conditions.) This can be visualized as taping the left and right edges of the rectangle to form a tube, then taping the top and bottom edges of the tube to form a torus (doughnut shape). Universes of other dimensions are handled similarly. This is done in order to solve boundary problems with neighborhoods. For example, in a 1-dimensional cellular automaton like the examples below, the neighborhood of a cell xit—where t is the time step (vertical), and i is the index (horizontal) in one generation—is {xi?1t?1, xit?1, xi+1t?1}. There will obviously be problems when a neighbourhood on a left border references its upper left cell, which is not in the cellular space, as part of its neighborhood. Stanis?aw Ulam, while working at the Los Alamos National Laboratory in the 1940s, studied the growth of crystals, using a simple lattice network as his model. At the same time, John von Neumann, Ulam"s colleague at Los Alamos, was working on the problem of self-replicating systems. Von Neumann"s initial design was founded upon the notion of one robot building another robot. This design is known as the kinematic model. As he developed this design, von Neumann came to realize the great difficulty of building a self-replicating robot, and of the great cost in providing the robot with a "sea of parts" from which to build its replicant. Ulam suggested that von Neumann develop his design around a mathematical abstraction, such as the one Ulam used to study crystal growth. Thus was born the first system of cellular automata. Like Ulam"s lattice network, von Neumann"s cellular automata are two-dimensional, with his self-replicator implemented algorithmically. The result was a universal copier and constructor working within a CA with a small neighborhood (only those cells that touch are neighbors; for von Neumann"s cellular automata, only orthogonal cells), and with 29 states per cell. Von Neumann gave an existence proof that a particular pattern would make endless copies of itself within the given cellular universe. This design is known as the tessellation model, and is called a von Neumann universal constructor. In the 1970s a two-state, two-dimensional cellular automaton named Game of Life became very widely known, particularly among the early computing community. Invented by John Conway, and popularized by Martin Gardner in a Scientific American article, its rules are as follows: If a black cell has 2 or 3 black neighbors, it stays black. If a black cell has less than 2 or more than 3 black neighbors it becomes white. If a white cell has 3 black neighbors, it becomes black. Despite its simplicity, the system achieves an impressive diversity of behavior, fluctuating between apparent randomness and order. One of the most apparent features of the Game of Life is the frequent occurrence of gliders, arrangements of cells that essentially move themselves across the grid. It is possible to arrange the automaton so that the gliders interact to perform computations, and after much effort it has been shown that the Game of Life can emulate a universal Turing machine. Possibly because it was viewed as a largely recreational topic, little follow-up work was done outside of investigating the particularities of the Game of Life and a few related rules. In 1969, however, German computer pioneer Konrad Zuse published his book Calculating Space, proposing that the physical laws of the universe are discrete by nature, and that the entire universe is just the output of a deterministic computation on a giant cellular automaton. This was the first book on what today is called digital physics. In 1983 Stephen Wolfram published the first of a series of papers systematically investigating a very basic but essentially unknown class of cellular automata, which he terms elementary cellular automata (see below). The unexpected complexity of the behavior of these simple rules led Wolfram to suspect that complexity in nature may be due to similar mechanisms. Additionally, during this period Wolfram formulated the concepts of intrinsic randomness and computational irreducibility, and suggested that rule 110 may be universal—a fact proved later with the help of Wolfram"s research assistant Matthew Cook in the 1990s. Wolfram left academia in the mid-late 1980s to create Mathematica, which he then used to extend his earlier results to a broad range of other simple, abstract systems. In 2002 he published his results in the 1280-page text A New Kind of Science, which extensively argued that the discoveries about cellular automata are not isolated facts but are robust and have significance for all disciplines of science. Despite much confusion in the press and academia, the book did not argue for a fundamental theory of physics based on cellular automata, and although it did describe a few specific physical models based on cellular automata, it also provided models based on qualitatively different abstract systems. In his 2005 book, The Lifebox, The Seashell and The Soul, Rudy Rucker expanded upon Wolfram"s theories toward a theory of Universal Automatism. This used cellular automata as a model to explain how simple rules can generate complex results. The simplest nontrivial CA would be one-dimensional, with two possible states per cell, and a cell"s neighbors defined to be the adjacent cells on either side of it. A cell and its two neighbors form a neighborhood of 3 cells, so there are 2³=8 possible patterns for a neighborhood. There are then 28=256 possible rules. These 256 CAs are generally referred to using Wolfram notation, a standard naming convention invented by Wolfram. The name of a CA is the decimal number which, in binary, gives the rule table, with the eight possible neighborhoods listed in reverse counting order. For example, below are tables defining the "rule 30 CA" and the "rule 110 CA" (in binary, 30 and 110 are written 11110 and 1101110, respectively) and graphical representations of them starting from a 1 in the center of each image: A table completely defines a CA rule. For example, the rule 30 table says that if three adjacent cells in the CA currently have the pattern 100 (left cell is on, middle and right cells are off), then the middle cell will become 1 (on) on the next time step. The rule 110 CA says the opposite for that particular case. A number of papers have analyzed and compared these 256 CAs, either individually or collectively. The rule 30 and rule 110 CAs are particularly interesting. Rule 30 generates apparent randomness despite the lack of anything that could reasonably be considered random input. Wolfram proposed using its center column as a pseudorandom number generator (PRNG); it passes many standard tests for randomness, and Wolfram uses this rule in the Mathematica product for creating random integers. (In particular, in the 1990s a cryptography survey book claimed that rule 30 was equivalent to a linear feedback shift register (LFSR), but in fact the claim was about rule 90.) Although Rule 30 produces randomness on many input patterns, there are also an infinite number of input patterns that result in repeating patterns. The trivial example of such a pattern is the input pattern only consisting of zeros. A less trivial example, found by Matthew Cook, is any input pattern consisting of infinite repetitions of the pattern "00001000111000", with repetitions optionally being separated by six ones. Rule 110, like the Game of Life, exhibits what Wolfram calls class IV behavior, which is neither completely random nor completely repetitive. Localized structures appear and interact in various complicated-looking ways. In the course of the development of A New Kind of Science, as a research assistant to Stephen Wolfram back in 1994, Matthew Cook proved that some of these structures were rich enough to support universality. This result is interesting because rule 110 is an extremely simple one-dimensional system, and one which is difficult to engineer to perform specific behavior. This result therefore provides significant support for Wolfram"s view that class IV systems are inherently likely to be universal. Cook presented his proof at a Santa Fe Institute conference on Cellular Automata in 1998, but Wolfram blocked the proof from being included in the conference proceedings, as Wolfram did not want the proof to be announced before the publication of A New Kind of Science. In 2004, Cook"s proof was finally published in Wolfram"s journal Complex Systems (Vol. 15, No. 1), over ten years after Cook came up with it. Rule 110 has been the basis over which some of the smallest universal Turing machines have been built, inspired on the breakthrough concepts that the development of the proof of rule 110 universality produced. --------------------------------------------------------------------------------------------------------------------------- -------------------------------------------------------------------------------------------------------------------------------- به طورخلاصه برای پاسخ دادن به این سئوال بایدگفت :نوع تمرین ومطالعه قبل ازآزمون باید با ماهیت آزمون هماهنگی داشته باشد.برای اینکه این مفهوم بیشتر تشریح شودبه توضیح زیر توجه کنید.دروس به دسته تقسیم می شوند 1-بیشترتحلیلی 2-بیشتر توصیفی بیشترتحلیلی:اگردرسی نیازبه تمرین زیادبرای افزایش مهارت حل تمرین داشته باشدوبه عبارت دیگرخواندن آن به تنهایی دردی رادوا نکند ،آن درس تحلیلی است.مثل:ریاضیات،فیزیک ،عربی و... بیشترتوصیفی:درسی راکه باخواندن بیشترمی توان به تسلط بسیار بالایی دست پیداکردومعمولا به حل تمرین بسیارزیادنیازدارد،توصیفی گویند.مثل:زیست،ادبیات،معارف و... سئوال:چگونه برای یک آزمون توصیفی خود راآماده کنیم؟ پاسخ:علاوه برروش مطالعه باید مرحله بازگو کردن یاتوصیف کردن (recite)راخیلی انجام دهید،به عبارت دیگر:تیترمطالب رانگاه کرده وسعی کنیدنکات آن پاراگراف رابگوییدوسپس بازگشته ونکات جاافتاده راباروش دیگر مطالعه کنید.چون اگرروش قبلی مطالعه خود راتکرارکنید.بازهم آن رانخواهیدآموخت ویافراموش خواهید کرد. به عبارت دیگربرای تسلطروی مباحث توصیفی بایدخروجی های شفاهی زیادی ازخودبگیریم.دراینجاخروجی یعنی پاسخگویی مطالب باکمک آموخته های ذهنی خود،علاوه براین،بایدباید زمان بندی ومرورهم به خوبی رعایت شود پاسخ:خروجی گرفتن وافزایش قدرت پاسخگویی دراین دروس با زیادخواندن به دست نمی آید درچنین دروسی بایدتمرین نوشتاری (حل تمرین)بیشتری انجام دادواین کار هرقدرتدریجی باشدنتایج بهتری به دنبال خواهد داشت. مثلا هگر دانش آموزی روزانه 5تا10تمرین فیزیک حل کند،به زودی دراین درس جزوبهترین های کلاس خود خواهدشد،درصورتی اگراین تمرین رایک جا قبل ازامتحانات حل کند.چنین رشد قابل توجهی نخواهد شد.
BurnAware Free 2.3.2
BurnAware Free 2.3.2
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