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Description Sets the type of endings that are put on lines The choices are butt, round, and square A value of butt indicates that there is a flat edge at the end of the specified line A value of round adds a semicircle with a diameter the width of the line to the end of the line A value of square adds a rectangle with a width half of the line s width and a length equal to the line s width at the end of the line The default is butt Sets the type of corners that occur when two lines meet The choices are miter, bevel, and round On all joins, a filled triangle connecting the two lines is connected A value of bevel uses only this filled triangle A value of miter indicates that in addition to the triangle, a second filled triangle is created The second triangle consists of a line that connects the two lines as well as the two lines themselves extended until they meet A value of round indicates that corners should be rounded when lines meet The arc has a diameter equal to the width of the line The default is miter Sets the width of the lines The default value is 1 Sets the max length that a line will be extended if lineJoin is set to miter If the length necessary to join the lines is greater than the miterLimit, the join will not occur The default is 10

void test() { Inner inner = new Inner(); innerdisplay(); } // this is an inner class class Inner { void display() { Systemoutprintln("display: outer_x = " + outer_x); } }

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oscillations of infinitesimal amplitude and a consequent dissipative effect However, one may imagine a process wherein small mass increments are removed one after another at a rate such that the piston's rise is continuous, with minute oscillation only at the end of the process The limiting case of removal of a succession of infinitesimal masses from the piston is approximated when the masses m in Fig 22 are replaced by a pile of powder, blown in a very fine stream from the piston During this process, the piston rises at a uniform but very slow rate, and the powder collects in storage at ever higher levels The system is never more than differentially displaced from internal equilibrium or from equilibrium with its surroundings If the removal of powder from the piston is stopped and the direction of transfer of powder is reversed, the process reverses direction and proceeds backwards along its original path Both the system and its surroundings are ultimately restored to their initial conditions The original process is reversible Without the assumption of a frictionless piston, we cannot imagine a reversible process If the piston sticks because of friction, a finite mass must be removed before the piston breaks free Thus the equilibrium condition necessary to reversibility is not maintained Moreover, friction between two sliding parts is a mechanism for the dissipation of mechanical energy into internal energy This discussion has centered on a single closed-system process, the expansion of a gas in a cylinder The opposite process, compression of a gas in a cylinder, is described in exactly the same way There are, however, many processes which are driven by the imbalance of forces other than mechanical forces For example, heat flow occurs when a temperature difference exists, electricity flows under the influence of an electromotive force, and chemical reactions occur because a chemical potential exists In general, a process is reversible when the net force driving it is only differential in size Thus heat is transferred reversibly when it flows from a finite object at temperature T to another such object at temperature T - d T.

Example contextlineCap = "round";

class InnerClassDemo { public static void main(String args[]) { Outer outer = new Outer();

contextlineJoin = "round";

(1183)

contextlineWidth = 5; contextmiterLimit = 1;

- 129 -

which follows from Eq (1182) and Eq (63), the definition of G The definition of M E is analogous to the definition of a residual property as given by Eq (641) Indeed, excess properties have a simple relation to residual properties, found by subtracting Eq (641) from Eq (1182):

TABLE 3-16

outertest();

Description Sets the size of the blurring effect The default value is 0 Sets the color of the shadow The default is transparent black Sets the distance that the shadow will be offset in the horizontal direction The default value is 0 Sets the distance that the shadow will be offset in the vertical direction The default value is 0

Since an ideal-gas mixture is an ideal solution of ideal gases, Eqs (1176) through (1179) become expressions for Mig when Mi is replaced by M ~ ! ~ example, Eq (1176) becomes: For

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