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Stanley Schachter (1971) put forward three general propositions: (a) Given a state of physiological arousal for which an individual has no immediate explanation, he will describe his state in terms of whatever cognitions are available (b) Given a state of physiological arousal for which an individual has a completely appropriate explanation, no evaluative needs will arise and the individual is unlikely to label his feelings in terms of (any) cognitions available (c) Given the same cognitive circumstances, the individual will react emotionally or describe his feelings as emotions only to the extent that he experiences a state of physiological arousal In other words, both physiological arousal and cognitive evaluation are necessary, but neither is a suf cient condition for the production of emotional states The main contribution of Schachter s group in the 1960s was in opening up a new era of investigation and theory.



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It rede ned the psychology of emotion just as James had done 70 years earlier The contribution was not so much the ingenious experiments but a straightforward statement of a visceralcognitive theory Visceral action was setting the stage for emotional experience, but so was a cognitive evaluation, and emotion was the product of the two Perhaps more important was the statement that general autonomic arousal rather than a speci c pattern was the visceral concomitant of emotional experience The consequences of this position have been a large number of experimental studies showing the in uence of visceral and cognitive factors ranging from the instigation of aggressive behavior to the occurrence of romantic love In the rst set of experiments, Schachter and Singer (1962) gave subjects injections of adrenaline under the cover story that these were vitamin compounds that would affect visual skills.

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In the Chapman-Enskog approach, increasingly higher-order derivatives and products of lower-order derivatives of the hydrodynamic fields occur in proceeding with the expansion By including these higher-order derivatives, the range of validity is not extended to shorter length and time scales; one can only expect further improvements where the Navier-Stokes equations already work well Additional features of the Boltzmann equation at short length and time scales can only be captured by considering further coarse-grained variables in addition to the hydrodynamic ones The idea underlying Grad's method is to use a class of trial solutions that contains a certain number of parameters in addition to the hydrodynamic fields p, o, and T These position-dependent parameters serve as the macroscopic fields of a coarse-grained level of description Time-evolution equations for the macroscopic fields are obtained as follows.

Following the injection, subjects were either informed of the consequences of the injection (ie, they were given correct information about the effects of adrenaline, but without having been told that they were given an adrenaline.

Transient analysis. The same variance relation (24.38) can be used to characterize the transient behavior of the filters, in addition to the following recursion for the mean weight-error vector (which follows by taking expectations of both sides of (24.31)):

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One chooses a number of low-order moments of the probability density in momentum space, and, for equal numbers of parameters and moments, one establishes a relationship between the parameters of the trial solutions and the moments in velocity space The time-evolution equations for the moments obtained from Boltzmann's equation are closed because one can eliminate higherorder moments by means of the explicit form of the trial solutions We thus arrive at time-evolution equations for the moments or, equivalently, for the parameters in the trial solutions, which are considered as the macroscopic fields The form of the trial solutions and the set of moments to be reproduced are the basic inputs of the method Unlike the Chapman-Enskog expansion, Grad's method is not based on a systematic expansion in a small parameter such as emfp.

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