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The audio output signal is provided at P1 through two capacitors C1 and C2, which are interfaced to your transceiver The output at P0 is the push to talk (PTT) line The output signal at P0 is fed to a 1-k resistor coupled to an npn transistor The transistor Q1 is used to drive the PTT relay which is used to turn on your ham radio transceiver, thus keying your radio A low-current reed relay is used to send Morse code Reed relays are very fast, have a long life, and consume low power, which is ideal for this application The PTT and audio output lines are brought out to the rear panel of the Morse code keyer and connected to a 1 8-in stereo jack You may wish install an external coaxial power jack on the rear panel as well.

The flywheel can be used as an energy reservoir, with energy being supplied at a slow constant rate or when it is available and being withdrawn when desired. A flywheel might, for example, be used to give good acceleration to an automobile that is underpowered by present standards. Regenerative breaking, power storage for peak-demand periods, and mechanical replacements for battery banks are all potential uses for the flywheel. The high charging and discharging rates of a flywheel system give it an advantage over other portable sources of power, such as batteries. Although the concepts developed in the previous sections are still true for energy-storage flywheels, the purpose is now to store as much kinetic energy, 0.5J 2, as possible. In most applications, the flywheel speed does not vary over 50 percent, so that only about 75 percent of this total energy is actually recoverable. The design of the ordinary flywheel is usually dictated by the allowable diameter, governed by the machine size, and the maximum speed, governed by the practicalities of a speedincreasing drive and higher bearing speeds. These constraints can result in a low peripheral speed, causing the economics to favor a rim-type flywheel design. The economics change with the energy-storage flywheel, since (1) larger values of total stored energy are usually involved, requiring heavier flywheels or more energy per unit weight of flywheel, (2) the weight of a heavy flywheel and the correspondingly heavy bearings and other components may be unacceptable, especially in mobile applications, and (3) the design constraints imposed in a machine where the flywheel limits the speed variation can be relaxed when the flywheel is the main component, encouraging optimization. Depending on the application, the energy per dollar, energy per weight, or energy per swept volume is usually maximized [7.1].

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7.4.1 Isotropic and Anisotropic Designs The stress equations for the thin disk given in Sec. 7.3.3 can be solved with r = t to give the shape for a fully stressed thin isotropic disk with no central bore: z = z0 exp 2 r2 2gSy (7.70)

OK, I have rambled on for quite a few pages about the whats and whys of particles. It is time to get your hands dirty with some code. First build a particle:

where Sy = allowable strength, for example, the yield strength of the material. Define the energy stored per unit weight as R = Fs Sy (7.71)

where Fs is a dimensionless factor that depends only on the shape of the flywheel. Using Eqs. (7.46) through (7.49), it turns out that the efficiency or geometric shape

You could build a cable with a 1 8-in stereo plug at one end and a suitable microphone connector at the opposite end of the cable The programming cable is connected to pins 1 through 4 of the BASIC STAMP 2 A 4-pin male header could be mounted on the circuit board for the programming cable A programming cable could be fabricated with a 4-pin female header and a length of flexible 4-conductor telephone cable connected to a 9-pin serial RS232 connector The Morse keyer can be powered by a 9-V transistor radio battery if desired; this would facilitate building a compact or portable unit Or the keyer could be powered from a 12-V system power bus.

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

Part 9:

@interface BBParticle : NSObject { BBPoint position; BBPoint velocity; CGFloat life; CGFloat size; CGFloat grow; CGFloat decay; }

This last section in the Third Edition provides the mechanical design engineer with the fundamental formulas for stress (Chap. 36) and deflection of beams (Chap. 37). This section also includes the stress and deformation of special geometries, such as curved beams and rings (Chap. 38), and the stress and deformation of pressurized cylinders (Chap. 39), which are developed as a result of internal pressure or from the effects of a press or shrink fit.

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