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Drag in a UIImageView from your Library as shown in Figure 6 69 and place it inside the View frame.

n You need different variations of an algorithm. n An algorithm uses data that is unknown to the client.

(7.15)

Example Code The following example Java code demonstrates the Strategy pattern:

While the screen is still active, go to your Image View Attributes window and select the einstein02.png image file, as shown in Figures 6 70 and 6 71. Save your work by entering S, and then return to Xcode.

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package javaee.architect.Strategy; public class StrategyPattern { public static void main(String[] args) { System.out.println("Strategy Pattern Demonstration."); System.out.println("-------------------------------"); // Construct strategies. System.out.println("Constructing strategies."); StrategyIF strategy1 = new ConcreteStrategy1(); StrategyIF strategy2 = new ConcreteStrategy2(); // Construct contexts. System.out.println("Constructing contexts."); Context context1 = new Context(strategy1); Context context2 = new Context(strategy2); // Execute contextInterface. System.out.println("Constructing context interfaces."); context1.contextInterface("J2EE Unleashed"); context2.contextInterface("J2EE Unleashed");

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With this in mind, we again follow the Noether procedure. Vary the action as if depended on the worldsheet coordinates, and look for terms multiplied by . At the end we consider to be constant so that term vanishes from the action the term which multiplies will be the energy-momentum tensor that we seek. We proceed in two parts. Let s take a look at the fermionic part of the lagrangian rst. We have i LF = 2 Using Eq. (7.15), we vary this term as follows: i i LF = ( ) ( ) 2 2 i i = ( ) ( ) 2 2 Let s apply the product rule and carry out the derivative on the second term: i i ( ) ( ) 2 2 i i i = ( ) 2 2 2 Now, the variation actually takes place as a variation of the action S, so we can integrate by parts. We do this on the last term to move one of the derivatives off . Integration by parts introduces a sign change, so we get i i i ( ) 2 2 2 i i i = ( ) + ( ) 2 2 2 i i i i = ( ) + + 2 2 2 2

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context1.contextInterface("The Secret Commissions"); context2.contextInterface("The Secret Commissions"); System.out.println(); } } package javaee.architect.Strategy; public class ConcreteStrategy1 implements StrategyIF { // Switch text to all upper case. public void algorithmInterface(String parm) { System.out.println(parm.toUpperCase()); } } package javaee.architect.Strategy; public class ConcreteStrategy2 implements StrategyIF { // Switch text beginning with "the". public void algorithmInterface(String parm) { System.out.println((parm.toLowerCase().startsWith("the ")) parm.substring (4)+ ", " + parm.substring(0,4) : parm); } } package javaee.architect.Strategy; public class Context { // Reference to the strategy. StrategyIF strategy; // Register reference to strategy on construction. public Context(StrategyIF parm) {this.strategy = parm;} // Call strategy's method. public void contextInterface(String parm) {strategy.algorithmInterface(parm);} } package javaee.architect.Strategy; public interface StrategyIF { public void algorithmInterface(String parm); }

The divergence term is not going to contribute anything, so we drop it. The rst and third terms cancel, leaving us with i LF = 2 This is what we want, because terms that multiply are going to be terms that make up the energy-momentum tensor T . This isn t quite right, because we want it to be symmetric. So, we take i i LF = 4 4 (7.16)

The Template Method pattern s intent is to define the skeleton of a function in an operation, deferring some steps to its subclasses. The Template Method lets subclasses redefine certain steps of a function without changing the structure of the function. The HttpServlet does this in the servlet API. The UML is shown in Figure 5-22.

Go back to Xcode, open up your Classes folder, open a file, and Enter so we can run it as shown in Figure 6 72.

In the Quiz, you will derive an expression for the bosonic part of the energy-momentum tensor. When all is said and done i i T = X X + + ( Trace ) 4 4 (7.17)

FIGURE 5-22

The Trace is explicitly removed to ensure that T remains traceless as required for scale invariance. The energy-momentum tensor and supercurrent can be written compactly using worldsheet light-cone coordinates. The energy-momentum tensor has two nonzero components given by i T++ = + X + X + + + + 2 The components of the supercurrent are

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