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'MORSE2.BS2 ' four message keyer for Amateur Radio. 'Richard Clemens, KB8AOB 'The user can input four different messages in msg1-msg4, 'their character counts in msc1-msc4, and use four 'buttons to display the output and/or key a transmitter. 'NB: the messages are limited to the upper and lower case 'letters, digits 0-9, space, period, comma, and / 'load the EEPROM with data 'switch, special characters, A-M, N-Z, and 0-9 '(switch is so we only convert data after an initial load) swtc data 0 spec data 0,87,207,54,149 leta data 66,132,164,131,1,36,195,4,2,116,163,68,194 letn data 130,227,100,212,67,3,129,35,20,99,148,180,196 nums data 253,125,61,29,13,5,133,197,229,245 'user can change the messages below msg1 data "CQ CQ CQ de KB8AOB KB8AOB KB8AOB K" msg2 data "QTH QTH is Buckhannon, WV Buckhannon, WV" msg3 data "UR RST RST is 599 599 NAME NAME HR IS RICH RICH" msg4 data "TNX for QSO and 73 de KB8AOB" 'character counts must match messages above msc1 con 34 msc2 con 40 msc3 con 48 msc4 con 28 tabl con 41 tone con 1200 spc con 380 dit con 70 dah con 210 chr var b0 ele var b1 x1 var b2 x2 var b3 x3 var b4 x4 var b5 'initialize pins 0 and 1 for output high 0 low 1 'clear the button variables b8 = 0 b9 = 0 b10 = 0 b11 = 0 'test to see if we just downloaded, if yes, set the 'switch so we don't try this again and then convert all 'the messages into their morse code bytes read 0,chr if chr <> 0 then loop write 0,255 'using the ASCII codes to shorten the lookdown 'replace each character with its morse code byte

Readers will note a difference in the style and character of the figures in this chapter. When this manuscript was received, the illustrations, all conceived and executed by Professor Torfason, were seen to be original and unique. We asked for and received from the publishers special permission to reproduce them exactly as they were drawn EDS.

2.3 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.

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factor Fs = 1.0 for the fully stressed profile. As Eq. (7.70) indicates, this profile has an infinite outer radius; truncating the profile reduces Fs substantially. Modifying the profile can improve the efficiency, increasing Fs to 0.97 (see Table 7.6), but that is the limit for a homogeneous isotropic design. To avoid this basic limitation and to take advantage of the higher strength-to-weight and stiffness-to-weight ratio of composite materials, recent efforts have concentrated on anisotropic designs ([7.1], [7.8]). Figure 7.7 describes a few of the many designs that are being developed.

This is a very basic particle. The basic state is position, life, and size. velocity, grow, and decay are the state changers. Particles can be far more complicated than this, and you will add some more stuff to your particle later, but for now let s keep it simple. Next you look inside your particle implementation:

7.4.2 Special Considerations Energy-storage flywheels have special problems which are related to their high speed, flexibility, and anisotropy. The increased operational speed requires highspeed power transmission and bearings as well as special attention to drag forces and the critical vibration speeds of the torsional system. A continuously variable transmission and operation in a vacuum are usually required. Forward whirling is a potentially serious problem that may limit the operating range or require external damping [7.3]. The flexibility can cause flywheel vibration modes with frequencies in the operating range and can also cause significant imbalance to occur as the flywheel deforms with speed. Anisotropy can cause failure in the weak direction (matrix failure or delamination) before the full strength in the strong direction is utilized.

Listing 12-1

7.5.1 Materials Neglecting gravity and other secondary loads, the stresses in a flywheel will be proportional to V 2 = (ro )2. Two flywheels of the same design but of different size will therefore have the same rim stress when their rim velocities are equal. Also, since the stress is proportional to V 2, a 10 percent increase in rotational speed will cause a 21 percent increase in stress. Although the strengths of flywheel materials are sometimes given in terms of their maximum rim velocities, these strengths include generous factors of safety to account for all the possible variations in the material properties, design details, and methods of manufacture. A rational approach would

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.

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