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A suggestion regarding advertising could be that clear guidelines for a transparent application of mobile advertising are established by the industry Such guidelines would, for example, describe how customers could opt-in or opt-out of advertising content, how providers would safeguard sensitive customer information or how much advertising a customer might expect A similar recommendation can be given to regulatory and legal institutions, to make privacy legislation as clear as possible in order to aid development of the mobile advertising market 944 Challenges for the Mobile-extension Model in Two Extreme Scenarios The third generic business model adds mobility to existing service offerings and solutions to existing user segments The main challenges are found in the product/service component and the processes component The key in this modelling task is to adapt new mobile possibilities to business and consider what kind of ties the service promises, user segments, processes, etc.





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By the law of large numbers, we would expect Xn to be close to q for large n. Sanov s theorem deals with the probability that pXn is far away from q. In particular, for concreteness, if we take p > q > 1 , Sanov s theorem states that 2 1 log Pr (X1 , X2 , . . . , Xn ) : X n p n p 1 p p log + (1 p) log q 1 q = D((p, 1 p)||(q, 1 q)). Justify the following steps:

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In a multiemitter structure, assuming the collector-to-emitter voltage is the same, hence Pk IC k VCE Hence, the general expression for temperature in a given emitter structure in tensor representation can be presented as follows, Tj TA yjk IC k VCE In the analysis, Liu and Khatibzadeh [41] represented the transistor as having a local thermal resistor element associated with each emitter, Rth, and substrate thermal resistor element, (Rth)sx. In this case, the substrate thermal resistance is common to all emitters in the multiple emitter structure. As a result, the thermal coupling is contained in the substrate thermal resistance element, (Rth)sx. Given two emitters, this can then be represented as the sum of the power in the self-emitter thermal resistance and power in the substrate thermal resistance, T1 TA Rth 1 IC1 VCE Rthsx IC1 VCE IC2 VCE T2 TA Rth 2 IC2 VCE Rthsx IC1 VCE IC2 VCE or, T1 TA Rth1 Rthsx IC1 VCE Rthsx IC2 VCE T2 TA Rthsx IC1 VCE Rth2 Rthsx IC2 VCE or in matrix form, T1 TA T2 TA ! Rth1 Rthsx Rthsx Rthsx Rth2 Rthsx ! IC1 VCE IC2 VCE !

countenanced a range of dream motives other than wishes, such as anxiety, though ultimately still rooted in childhood (p 8) But this modification did not remedy the fundamental epistemological defect in the claim that the method of free association can reliably identify dream motives Undaunted, Arlow and Brenner (1988, p 8) declare: The theory and technique of dream analysis [by free association] in no way differs from the way one would analyze a neurotic symptom, a parapraxis, or any other object of [psycho]analytic scrutiny By the same token, these analysts insouciantly announce: Dreams are, in fact, compromise-formations like any others (pp 7 8) Yet this ontological conclusion is predicated on the ill-founded epistemological thesis that free associations reliably identify repressions to be the causes of symptoms, dreams, and slips.

derive the ratio of the power of the maximum power of a gallium arsenide device and silicon germanium device Assuming the same unity current gain cutoff frequency, derive the relationship between the two power values 5 Derive a relationship of a GaAs HBT in a diode con guration used in a diode string Assume N GaAs HBT devices in series 6 Derive a relationship of a trigger network consisting of N GaAs HBT diode-con gured elements in series with an open-base GaAs HBT in a collector-to-emitter con guration Compare this to a trigger network of M SiGe HBT diode-con gured elements in series with an open-base SiGe HBT (in a common-emitter con guration) Compare the two trigger voltages Show the ratio of the two devices Assuming the same trigger voltage condition, derive the relationship between the N GaAs HBT devices and the M SiGe HBT devices 7.

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