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In the International System (SI), m is expressed in kilograms and r in metres, with I (moment of inertia) having the dimension kilogram-metre square.
We assume that all grains are spherical with material density s; thus, the grain mass m is expressed as.
In addition, the universal formula of R m is expressed as (Jia et al. 2007) R_{text{m}} = frac{{A_{text{eff}} }}{{P_{text{eff}} }}.
The full time t = t ^ + t m is expressed as the form of the fast time t ^ and the slow time t m = m ⋅ PRI, where m are integers and PRI is the pulse repetition interval.
The moment-rotation relationship is given as theta_{text{r}} = 1.64 times 10^{3} left( {KM} right) + 1.03 times 10^{14} left( {KM} right)^{3},+,8.18 times 10^{25} left( {KM} right)^{5}, (1 where moment (M) is expressed in kNm and all other size parameters are expressed in mm.
Since it is assumed that the received symbol/codeword sequence is corrupted by white Gaussian noise, the probability of receiving r t and time instant t having transmitted d t ( m ), is expressed as [1, 2, 6, 7, 11] P ( r t | d ( m ) ) = 1 2 π σ exp − | Δ t ( m ) | 2 2 σ 2, (2).
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Further, from the η−μ fading distribution, the Nakagami-m model could be obtained in two cases: first, for η→1, with parameter m being expressed as m=μ/2 and second, for η→0, with parameter m being expressed as m=μ.
Furthermore, the results for the blade diameter 0.78 and 0.80 m are expressed by Figs. 8 and 9, respectively.
In Proposition 2.3, the minimality (while satisfying inefficiency) of the presentation P M was expressed in (7).
O q and α m are expressed from the tension T and the perturbed vocal effort E p (defined in Section 4.2.1).
Conservation integrals also have the similar analogy between anisotropic and isotropic elasticity so that J integral and J-based mutual integral M are expressed in the same complex forms for anisotropic and isotropic materials, when both end points of the integration paths are on the straight interface.
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