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do { Console.Write("."); Thread.Sleep(100); } while (mt1.Thrd.IsAlive && mt2.Thrd.IsAlive && mt3.Thrd.IsAlive); Console.WriteLine("Main thread ending."); } }
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The term transparent appropriately describes a transparently bridged network: the devices connected to the network are unaware that the bridge, or switch, is a part of the network and is forwarding frames to destinations. Basically, transparent-bridge networks physically look like a bunch of star topologies connected together. However, transparent bridges give the appearance to connected devices that every device in the broadcast domain is on the same logical segment, as shown in Figure 4-2. The following sections cover the three main functions of transparent bridges and switches in more depth. As you read through these sections, you ll see the term switch used to describe the layer 2 device; however, the terms bridge and switch are interchangeable when it comes to the three main functions.
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Recall that typeof returns a Type object that represents the specified type, which in this case is MyClass. Using t and the Reflection API, the program then displays information about the methods supported by MyClass. First, a list of the methods is obtained by the following statement:
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If you had a horseshoe-shaped magnet with the ends close together and you moved a wire through its pole are at a right angle to the flux as shown in Figure 6-1, the equation describing it would be V 5 Blv 3 10 8 In this equation, a simplified form of Faraday s Law, V is the induced voltage in volts, B is the flux density in lines per square inch, 1 is the length of that part of the conductor actually cutting the flux, and v is the velocity in inches per second. For example, if you moved a 1-inch wire or conductor at a right angle to a field of 50,000 lines per square inch at 50 feet per second, V 5 50000 3 1 3 50 3 12 3 10 8 5 0.3 volts This relationship holds true whether the field is stationary and the wire is moving or vice versa. The faster you cut the lines of flux, the greater the voltage, but you must do so at right angles. (At any angle f other than the 90-degree right angle, that equation becomes V 5 Blv 3 sin f3 10 8.) What you have just demonstrated is Faraday s Law or the generator rule: Motion of a conductor at a right angle through a magnetic field induces a voltage across the conductor. If the circuit is closed, the induced voltage will cause a current to flow. A handy way to remember the relationships is the right-hand rule: the thumb of your right hand points upward in the direction of the motion of the conductor, your index finger extends at right angles to it in the direction of the flux (from north to south pole), and your third finger extends in a direction at right angles to the other two, indicating the polarity of the induced voltage or the direction in which the current will flow as shown in Figure 6-1. The flip-side or corollary to the generator rule is the motor rule whose equation is V 5 0.885 3 BI 3 I 3 10 8 where F is the force generated on the conductor in pounds, B is the flux density in lines per square inch, 1 is the length of that part of the conductor actually cutting the flux, and I is the current in amperes. For example, if you had a 1-inch wire at right angles to a field of 50,000 lines per square inch with a current of 100 amperes flowing through it: V 5 0.885 3 50000 3 1 3 100 3 10 7 5 0.44 pounds What we have just demonstrated here is Ampere s Law or the motor rule: Current flowing through a conductor at a right angle to a magnetic field produces a force upon the conductor. The right-hand rule is again a handy way to remember the relationships, but this time the thumb of your right hand points toward you in the direction of the current through the conductor, your extended index finger at right angles to it points in the direction of the flux (from north to south pole), and your extended third finger points downwards in a direction at right angles to the other two, indicating the direction of the generated force as shown in Figure 6-1. Now you re ready to talk seriously about motors.
Recordable CDs differ in some important ways from standard, mass-replicated CDs. When a blank, recordable CD is positioned in a recorder for the rst time, a spiral groove is already embedded in the polycarbonate substrate, indicating the path that the CD recorder laser head will track while burning the data pattern. Instead of the aluminum layer used in standard CDs, a recordable CD has a ne gold layer. Gold not only offers a highly re ective surface, but it resists corrosion much more effectively than aluminum. Another layer, composed of an organic dye sandwiched between the polycarbonate substrate and the gold layer, serves as the recording medium. As with standard CD-ROMs, a protective lacquer surface provides a degree of scratch resistance and durability to the outer layers of the disc. Figure 2 - 3 compare the materials used in the layers for CD-ROM discs and CD-R discs.
Since a file s date and time are generally used to indicate the time of the file s last modification, you should use setftime( ) carefully. If setftime( ) is successful, 0 is returned. If an error occurs, 1 is returned and errno is set to one of the following: EINVFNC EACCES EBADF Invalid function number Access denied Bad file handle
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STRENGTHENING AND REPAIR WORK
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C# 3.0: A Beginner s Guide
The basic building block of R/C models is the R/C servo. Usually packaged along with a radio transmitter and receiver set, an R/C servo is a miniature electronics device that includes an electronic motor-controller board, a motor, a geartrain, and a position-feedback sensor all in one small plastic case. The servo contains a simple electronic circuit. Originally made from discrete components but now packaged in a single custom integrated circuit, the servo converts the length of the input pulse into a voltage level, compares the voltage level to the signal from the position sensor on the output shaft, and drives the motor appropriately depending on the difference. The effect is that the signal from the radio controls the position of the output shaft of the servo. Typical R/C servos have a range of travel from 90 to 120 degrees, with a 2.0-millisecond pulse driving the shaft fully clockwise and a 1.0-millisecond pulse driving it fully counterclockwise. Most servos have a maximum range of travel of about 180 degrees, but the pulse-width range will be from 0.8 to 2.2 milliseconds to achieve this range of motion. In the early days of R/C hobbies, all controls worked through mechanical servos. R/C servos directly drove steering links in cars and control surfaces on model airplanes. Throttle control of motors was also accomplished with servos. A servo would open and control the intake valve on a gas engine to control its power. When electric motors became popular in R/C cars, the same hobby control servos were used to control them; but instead of opening and closing a throttle valve, the servo arm would slide along a set of contacts to make or break the power circuit to the motor. When Field Effect Transistor (FET) type electronic speed controllers entered the market, they duplicated the interface of the earlier mechanical speed controllers, with what had been a position control signal to control a servo s output shaft now being a speed and direction control for an electric motor.
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