By Michele Carter
A behind-the-scenes exploration of the Dungeons & Dragons(R) game.This lavishly illustrated ebook offers roleplaying online game lovers a special, behind-the-curtain glimpse into the making of the Dungeons & Dragons roleplaying online game. The ebook includes essays and asides from the game's prime designers, builders, and editors. via phrases and illustrations, it explores the various D&D game's so much iconic races and periods, sharing insights by no means prior to published in any prior video game product.
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Extra info for Behind the Screen: Races and Classes (Dungeons & Dragons)
The slope of the straight line, which is obtained, if the right temperature range is chosen, gives the value of a. In Fig. 7 this is demonstrated for an industrial PP. The cooling rates are indicated near the curves. The expected linearity and parallelism is clearly shown. The slight curvatures at the lower ends must be ascribed to small errors in the base line position. e. g ¼ 10 mWKÀ1. This fact can easily be explained: In  metals were used for the samples. As the heat conductivities of these samples is factors of about 400 higher than that of the polymer, the obtained heat transfer coefficient is higher and practically equal to the coefficient for the transfer between pan and furnace.
1) for bypassing crystallization. This result seems to fit nicely into the picture delivered by Fig. 10. The fact that the peaks become broader and lower with decreasing temperature of the maximum, can have various reasons. There is the heat transfer problem which, however, cannot easily be solved because of the fact that the sample experiences two heat flows, one from the heater and the other to the gas of constant low temperature. But there is also a possible influence of changing crystallization kinetics with decreasing temperature.
It will turn out that with higher cooling rates a correction of the peak temperature becomes unavoidable, as also Eder has shown. As already announced, the temperature Ts in the sample becomes quite different from the furnace temperature Tf at the maximum of the DSC-curve. 67) The sum of the second term and the third term of this equation can give quite a temperature rise above the furnace temperature. This becomes evident for the high cooling rate of 100 KminÀ1. In fact, with the aid of this equation the transformation from Tf to Ts was carried out on the abscissa of Fig.