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Two values of the gap are considered: 0·01D and 0·075 D, where D is the diameter of the main cylinder.
Low values of the gap (ΔE = ELUMO – HOMO), will render good inhibition efficiencies since the energy to remove an electron from the last occupied orbital will be minimized.
At such low speed, the difference between the values of the gap (G) and headway (D) becomes quite significant which is explained in Fig. 6.
For smaller gaps the pumped flux reduction is found to be negligible, while for large values of the gap width the pumped flux reduction may reach the value of 20%.
Explicit analysis and prediction algorithms are described for arbitrary values of the gap number N. It is found that the method with N ∼ 10 is computationally inexpensive and provides a useful analysis for a class of problems likely to occur in experimental situations.
So, considering the average length of the leading vehicle (vehicle-1) to be 4.343 m (IRC: SP-41), and speed of the vehicle as 20 km/h, values of the gap have been found to be about 0.78 s lower than headway values.
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Calculation considers single mean values of the gap-acceptance parameters, neglecting the inherent variations in these random variables and providing a single value of entry capacity.
The present value of the gap between America's long-term entitlement promises and its expected tax revenues looks to be more than $70 trillion.
The lower value of the gap means that the magnetic force was stronger.
In the example presented in Figure 2, the optimal value of the gap was 2.95 mm.
The value of the gap can be reproduced by assuming the occurrence of Coulomb blockade effects in graphene.
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