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int length( ) char charAt(int index) Here is a program that demonstrates these methods: // Demonstrating some String methods class StringDemo2 { public static void main(String args[]) { String strOb1 = "First String"; String strOb2 = "Second String"; String strOb3 = strOb1; Systemoutprintln("Length of strOb1: " + strOb1length()); Systemoutprintln("Char at index 3 in strOb1: " + strOb1charAt(3));

Gjd = r i ( T )+ RT Inxif,

3:

if(strOb1equals(strOb2)) Systemoutprintln("strOb1 == strOb2"); else Systemoutprintln("strOb1 != strOb2"); if(strOb1equals(strOb3)) Systemoutprintln("strOb1 == strOb3"); else Systemoutprintln("strOb1 != strOb3");

Name beginPath()

By difference,

Description Sets the subpath list to 0 Any paths set and undrawn at this point will not be displayed Connects the last point in the subpath to (x,y) using (cp1x, cp1y) and (cp2x, cp2y) as control points for a cubic B zier curve Creates a new clipping region by intersecting the current clipping region with the area defined in the current path Closes the last subpath and creates a new subpath that has the previous subpath s last point as its first point Fills any open subpaths and then closes them Uses the fillStyle to determine how the fill should appear Draws a line from the last point in the subpath to the point defined by (x, y) Creates a new subpath with the point (x, y) added to it Connects the last point in the subpath to (x,y) using (cpx, cpy) as the control point for a quadratic B zier curve Creates a new subpath containing the rectangle defined by starting point (x, y) with width w and height h Draws the strokes of the current path and display based on the settings specified by lineWidth, lineCap, lineJoin, miterLimit, and strokeStyle

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This program generates the following output: Length of strOb1: 12 Char at index 3 in strOb1: s strOb1 != strOb2 strOb1 == strOb3 Of course, you can have arrays of strings, just like you can have arrays of any other type of object For example: // Demonstrate String arrays class StringDemo3 { public static void main(String args[]) { String str[] = { "one", "two", "three" }; for(int i=0; i<strlength; i++) Systemoutprintln("str[" + i + "]: " + str[i]);

canvas Path API Methods (continued)

The left side of this equation is the partial excess Gibbs energy G; the dimensionless ratio : f, appearing on the right is the activity coeficient of species i in solution, symbol yi Thus, by definition,

Here is the output from this program: str[0]: one str[1]: two str[2]: three As you will see in the following section, string arrays play an important part in many Java programs

Example contextbeginPath();

- 133 -

390 Whence,

bezierCurveTo (cp1x, cp1y, cp2x, cp2y, x, y)

contextmoveTo(50,50); contextbezierCurveTo(65, 25, 85, 25, 100, 50);

Sometimes you will want to pass information into a program when you run it This is accomplished by passing command-line arguments to main( ) A command-line argument is the information that directly follows the program's name on the command line when it is executed To access the command-line arguments inside a Java program is quite easy they are stored as strings in the String array passed to main( ) For example, the following program displays all of the command-line arguments that it is called with: // Display all command-line arguments class CommandLine { public static void main(String args[]) { for(int i=0; i<argslength; i++) Systemoutprintln("args[" + i + "]: " + args[i]); } } Try executing this program, as shown here: java CommandLine this is a test 100 -1 When you do, you will see the following output: args[0]: args[1]: args[2]: args[3]: args[4]: args[5]: this is a test 100 -1

CHAPTER 11 Solution Thermodynamics: Theory (1188)

clip()

Note All command-line arguments are passed as strings You must convert numeric values to their internal forms manually, as explained in 14

context arc(150,150,100,0,Math PI*2,true); contextclip(); contextclosePath();

These equations establish a thermodynamic foundation for the activity coefficient, which appeared in Sec 105 as a factor introduced into Raoult's law to account for liquid-phase nonidealities Comparison with Eq (1147) shows that Eq (1188) relates yi to GE exactly as Eq (1147) relates $i to For an ideal solution, GE = 0, m therefore yi = 1 d An alternative form of Eq (1186) follows by introduction of the activity coefficient through Eq (1188):

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