M2L2 Set Theory and Event Operations 1. Introduction This lecture is a continuation of discussion on random events that started with definition of various terms related to random events and concepts of probability in previous lecture. Here Set Theory, its properties and various set or event operations are explained in detail with relevant examples. 2. Set Theory To understand Set Theory one should know the definition of ‘Set’ first. A Set is a collection of physical or mathematical objects called as members or elements. The elements of a set do not require to have any similarity among them except belong to the same set. Set Theory is the theory that is concerned with the properties of a set which are independent of particular elements belong to the set. For example, i. When a coin is tossed twice, the possible four outcomes or events and form the sample space, i.e. and T/T}. Any one or more than one possibility from S will form a set. ii. If an experiment is carried out to determine the strength of concrete for a number of concrete blocks, the all the experiment results will form a set. iii. If the stage height is recorded at a river gauging station, all the possible values of stage-height will form a set. 3. Set Properties The properties of Set Theory should be explored to understand and apply Set Theory in practical problems. Common properties are explained here with diagram. Property 1. Two different sets and are equal if all elements of the set ‘ ’ belong to set ‘ ’ and vice-versa. In diagram below (Fig. 1), ‘ ’ and ‘ ’ are two sets for which elements are completely overlapping each other. Fig. 1. Equal Sets Property 2. A set ‘ ’ is proper subset of another set ‘ ’ when all elements of set ‘ ’ belongs to ‘ ’, not vice-versa, it is denoted as: . In diagram below (Fig. 2) all the elements of set, ‘ ’ are enclosed by the boundary of set ‘ ’. However, the reverse is not true. Fig. 2. Subset Property 3. An empty or null set is defined as the set contains no elements, it is denoted as: . The diagram below (Fig. 3) shows a set ‘ ’ with no elements within its boundary. S Fig. 3. Null Set Property 4. A set is said to be ordered if a relation (‘ ’ or ‘ ’) for any two elements, so that a. either b. if or is possible. and b c , then . 4. Set Operations Several operations on sets or subset or events are possible, which are important in any analysis using random variables. 4.1. Union Union is an event operation when a set of elements are selected based on their occurrence in two sets ‘ ’ and ‘ ’ (belongs to set ‘ ’) following three alternative conditions: ‘ alone’, ‘ alone’, or both and . This operation is denoted by: (read as union ). The figure below (Fig. 4) shows that elements shaded in red denoted as ‘ ’ union ‘ ’ that consists of ‘ alone’ or in ‘ alone’, or in the overlapped area. Fig. 4. Venn diagram for Union 4.2. Intersection Intersection is an event operation when a set of elements are selected based on their occurrence in both the sets - ‘ ’ and ‘ ’ (belongs to set ‘ ’). This is denoted by: (read as intersection ). In figure, the overlapped area (shaded in yellow) of sets ‘ ’ and ‘ ’ are known as . Fig. 5. Venn diagram for Intersection 4.3. Mutually Exclusive Sets Two events ‘ ’ and ‘ ’ in set ‘ ’ are mutually exclusive when none of the outcomes in ‘ ’ belongs to ‘ ’ or vice-versa. These are denoted as: . Venn diagram for such condition is presented in fig. 6. There is no overlap between ‘ ’ and ‘ ’. Fig. 6. Venn diagram for Mutually Exclusive Sets 4.4. Collectively Exhaustive Sets When union of all subsets ,…. comprise the whole sample space, ‘ ’, then are called collectively exhaustive. These are denoted as: , . The visualization is provided in the figure below (Fig. 7). One important point to note that intersection of any two sets need not be null set. Fig. 7. Venn diagram for Collectively Exhaustive Sets 4.5. Partition of a Set Partition of a set, ‘ ’ is the collection of mutually exclusive and collective exhaustive subsets . It is denoted as: where, The visualization is provided below, it is to be noted that all the subsets for . are non-empty, non-overlapping events and the covering whole of set ‘ ’. . Fig. 8. Venn diagram for Set Partition 4.6. Complements Complements of a set ‘ ’ is the set of events in ‘ ’ that do not belong to ‘ ’. Complements of any event ‘ ’ are denoted as: . The visualization is provided in the fig. 9. Any event or subset, other than those within the boundary of ‘ ’, are complements of ‘ ’, denoted as A in the figure. Fig. 9. Venn diagram for Complement 4.7. De Morgan’s Law When in a set identity, all the subsets are replaced by their complements, all unions by intersections, and all intersections by unions, the identity is preserved. For example, if ‘ ’ and ‘ ’ are subsets of a set ‘ ’, then , ….…………………………..(1) Here, AB is shortened form of A B . The visualization for this example is provided in the following figure (Fig. 10). S Fig. 10. Example of De Morgan’s Law De Morgan’s Law for set operation can be expanded or demonstrated using three subsets, ‘ ’, ‘ ’ and ‘ ’, all belong to ‘ ’. With repeated application of the law, it can be denoted as: ………………………………..(2) Using the identity, , one can find for three subsets: ………………………………..(3) And, using the other identity, , one can get: ……………………………….(4) Similarly, ………………………….(5) Thus, applying De Morgan law on both sides of the Eqn. 2, one can get: ……………………………..(6) This is exactly the same taking Eqn. 3 for LHS and Eqn. 5 for RHS. One can draw a similar diagram for three subsets as shown here (Fig. 10) to understand the application of De Morgan’s Law. 4.8. Duality Principle This is basically an extension of De Morgan’s Law. Since it is known that for a set, ‘ ’, and , for identity like, Eqn. 6, if all the unions are replaced by intersections, all intersections by unions and the set ‘ ’ by and the set by , the identity is still preserved. Thus leads to . leads to 4.9. , similarly, Symmetric Difference For any two sets and , the set of elements which belongs to only one on the sets (not both) is called Symmetric Difference Set. The Venn diagram for visualization of this set operation is given in Fig. 11 below. Fig. 11. Symmetric Difference Set 4.10. Cartesian Product For any two set of events ‘ ’ and ‘ ’, a new set, that comprises all the possible ordered pair of elements belong to ‘ ’ and ‘ ’ ( ‘ ’. It is denoted as ) respectively, is called Cartesian product of ‘ ’ and . Here, an ordered pair is a collection of objects having two coordinates, such that one can uniquely determine any object. Thus, first coordinate is ‘ ’ and the second coordinate is ‘ ’ then the ordered pair is ( 4.11. ), which is not same as ( ). Power Set The Power Set of any set, ‘ ’ is the set whose elements are all possible subsets of ‘ ’ itself. e.g. Power Set of . is 5. Special Sets A set ‘ ’ is called open set if any point ‘ ’ in ‘ ’ always belongs to the set, even though it moves to some particular direction. The complement of an open set is called closed set. Example of open set and closed set are given in Fig. 12. The points ( ) satisfying the condition are coloured in blue. The points ( ) satisfying the condition are coloured in red. Any point within the area in red form an open set. Whereas, the union of red and black points, forms closed set. Fig. 12. Special Set [source: Wikipedia.org] 5.1. Borel Set Suppose is an infinite sequence of sets in ‘ ’. If the union and intersection of these sets also belongs to ‘ ’, then 5.2. is called a Borel Field or Set. Sigma-Algebra A - algebra of a set ‘ ’ is a non-empty collection Ω of subsets of S (including S itself) that is closed under complementation and countable unions of its members. e.g. if one possible - algebra on , is: 6. Probability Space Though Theory of Probability discussed already in previous lecture, here the relevance of it in set operations are described in brief. According to Theory of Probability, or Ω is called as certain event, its elements as experimental outcomes and its subsets as events. Here the empty set element is called as impossible event and the event consists of single only is called as an elementary event. It should be kept in mind that while applying Theory of Probability to physical problems, the identification of experimental outcomes is not always unique. A single performance of an experiment is called trial. 7. Concluding Remarks Set Theory defines the various interrelationships among the elements or subsets of a set. The set operations also classify various kinds of set properties of the elements. The details of Axioms of Probability that deals with probabilistic properties of events and sets will be discussed in the next lecture.
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