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The proof of equation (14) and various subsequent generalizations is much more difficult than that of the weak law of large numbers.
Proof of Equation 68.
Consequently, we complete the proof of equation (2.7).
We can also give another intuitive proof of equation (52) as follows.
end{aligned} (28) The proof of Equation (18) is the same way.
The detailed proof of Equation 17 is given in Appendix 6.1.
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Proof of Equations 19 and 20.
We are now ready to proceed with the proof of Equations (5), which is organized in three parts.
As in the proof of equations (3.3) and (3.8) above, we can show that lim sup n → ∞ 〈 C u n + λ v ∗, u n 〉 ≤ 0 and lim n → ∞ 〈 C u n + λ v ∗, y 〉 = 0. for every y ∈ L { F n }.
This chapter discusses fluid film bearings, together with a proof of Reynolds equation and also the relevance of the Navier Stokes equations for certain applications.
The proof of this equation is beyond the scope of this review and may be found in [ 83].
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