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A navigability arrow on an association shows which direction the association can be traversed or queried. An OrderDetail can be queried about its Item, but not the other way around. The arrow also lets you know who owns the association's implementation; in this case, OrderDetail has an Item. Associations with no navigability arrows are bidirectional. The multiplicity of an association end is the number of possible instances of the class associated with a single instance of the other end. Multiplicities, shown in the following table, are single numbers or ranges of numbers. In our example, there can be only one User for each Order, but a User can have any number of Orders.

In the header file, we told the computer that we are going to do some action(s) when a button is pressed. Now that we ve pasted this set of commands into the implementation file, we replace the ; with a set of brackets. It is inside these brackets that we will tell the computer what needs to be implemented when the button is pressed.

(relabel dummy indices, , )

0..1 0..* or * 1 1..*

So we ve established our rst fact to le away about the energy-momentum tensor for the string. It s traceless: T = 0 (3.5)

Zero or one instance; the notation n . . m indicates n to m instances No limit on the number of instances (including none) Exactly one instance At least one instance

#import "helloWorld_005ViewController.h" @implementation helloWorld_005ViewController - (IBAction)buttonPressed:(id) sender{ }

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In this section we will list some of the symmetries of the Polyakov action (and hence of the bosonic string in Minkowski space-time). There are three symmetry groups of the Polyakov action. These include Poincar transformations Reparameterizations of the worldsheet coordinates Weyl transformations The concept of symmetries is so important we will take a momentary digression to discuss the topic before describing the symmetries of the Polyakov action. Symmetries in physics can be global symmetries or local symmetries. These are de ned as follows: A global symmetry is one that holds at all points in space-time. The parameters of the transformation will not depend on space-time. A local symmetry is one that acts differently at different space-time points. In this case, the parameters of the transformation will be functions of the space-time coordinates. You should recall from your studies of classical mechanics and quantum eld theory that a symmetry in physics leads to a conservation law. The formal statement

Every class diagram has classes, associations, and multiplicities. Navigability and roles are optional items placed in a diagram to provide clarity. The class notation is a three-piece rectangle with the class name, attributes, and operations. Attributes and operations can be labeled according to access and scope. It is preferable that you name classes as singular nouns, such as User instead of Users. Static members are underlined, and Instance members are not. The operations follow this form: <access specifier> <name> ( <parameter list>) : <return type>. The parameter list shows each parameter type preceded by a colon. Access specifiers, shown in the following, appear in front of each member.

To simplify complex class diagrams, you can group classes into packages. A package is a collection of logically-related UML elements. The diagram shown in Figure 3-12 is a business model in which the classes are grouped into packages. Packages appear

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