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Einstein abandoned his constant, referring to it as his biggest blunder.
By using separation of variables, the wave equation can be written with spherical symmetry -y^{{primeprime} }(x)+omega(x y=lambda y, (1.1) where λ is a constant referring to the eigenvalue of the problem, and (omega(x)=omega_{o}(x)+frac{l(l+1)}{x^{2}}) [1], where l is a positive integer or zero and (omega_{o}(x)) will be defined in what follows.
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Dimensionless constant referred to as separation factor.
The R L is a dimensionless constant referred to as separation factor.
The essential features of the Langmuir isotherm may be expressed in terms of equilibrium parameter RL, which is a dimensionless constant referred to as separation factor or equilibrium parameter (Weber and Chakkravorti 1974): R L = 1 1 + bC 0. (14).
The essential features of the Langmuir isotherm may be expressed in terms of equilibrium parameter RL, which is a dimensionless constant referred to as separation factor or equilibrium parameter (Weber and Chakkravorti 1974): R_{text{L}} = frac{1}{{1 + bC_{0} }} (5).
The essential feature of the Langmuir isotherm may be expressed in terms of equilibrium parameter R L (Fig. 16b) which is a dimensionless constant referred to as separation factor or equilibrium parameter (Hao et al. 2010).
The essential features of the Langmuir isotherm may be expressed in terms of equilibrium parameter R L, which is a dimensionless constant referred to as separation factor or equilibrium parameter (Webber and Chakravarti 1974).
On the other hand, there are also close links between contractive self-mappings and Kannan self-mappings [2, 15 17] with constant (referred to in the following as Kannan self-mappings).
The essential features of the Langmuir isotherm may be expressed in terms of equilibrium parameter R L, which is a dimensionless constant referred to as separation factor: R_{text{L}} = frac{1}{{1 + K_{text{L}} C_{text{o}} }}.
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