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Table 2 IPC energy models according to message size IPC mechanism Energy model: E IPC (nJ) Average error Anonymous pipe 3068 × e 103. 9 ∗ 1 0 − 6 × msz 2.149 Named pipe 3003.

Equation (15) represents the energy model: E ipc ( msz ) = λ × e ( δ × msz ) (15) Figure 13 IPC energy variation as a function of message size.

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To characterize the power and energy consumption of IPC, we have to execute test programs, each one repeatedly calling an IPC mechanism.

Figure13 depicts the influence of the message size msz on the energy consumption of IPC: Eipc.

The potential energy of an IPC in the presence of the external field Φ z) can be expressed as 2where Qeff is the orientational dependent, effective charge of an IPC; Qeff can be read off from eqs 3 and 4 of ref (19) as 3where q e is the magnitude of the elementary charge, a ≡ e, θ is the angle with respect to the z-axis, and P2 l (cos θ) is the Legendre polynomial of order 2 l.

However, the IPC website makes it clear that the IPC is a Diageo/Guinness initiative.

Murry in 1986 showed that IPC caused no reduction in the amount of high energy phosphates in tissues [ 21] but surprisingly the amount of vitamin E in plasma of IPC group was significantly higher than that in the control group.

Columns 2 and 3 of Table 1 report the resulting particle particle interaction energies at contact for each of the IPC types; additionally, in panel b of Figure 1, the pair potentials for systems 45n and 45c are displayed.

In isothermal crystallization experiment, combining Avrami Method and Hoffman Lauritzen Model, it was found that the half-time of crystallization (t1/2) of pre-sheared IPC was greatly shortened and the calculated fold surface free energy (σe) within the isothermal temperatures investigated showed a large reduction.

DIM presents, on average, 2.7 times of performance gains and 2.35 times of energy savings over a MIPS processor, and a higher IPC than an out-of-order superscalar processor, running the MIBench benchmark set.

The self-assembly of the selected IPC systems under confinement was investigated in conditions such that the characteristic energy of the directional attractive interactions was much greater than the thermal energy.

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