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d() is the number of positive divisors of n, including 1 and n itself; σ() is the sum of the positive divisors of n, including 1 and n itselfs() is the sum of the proper divisors of n, including 1 but not n itself; that is, s(n) = σ(n) − n
A number where some but not all prime factors have multiplicity above 1 is neither square-free nor squareful. The Liouville function λ(n) is 1 if Ω(n) is even, and is -1 if Ω(n) is odd. The Möbius function μ(n) is 0 if n is not square-free. Otherwise μ(n) is 1 if Ω(n) is even, and is −1 if Ω(n) is odd.
For gases, departure from 3 R per mole of atoms is generally due to two factors: (1) failure of the higher quantum-energy-spaced vibration modes in gas molecules to be excited at room temperature, and (2) loss of potential energy degree of freedom for small gas molecules, simply because most of their atoms are not bonded maximally in space to ...
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L −1 M −1 T 3 Θ: intensive Viscosity: η: The measure of the internal friction in a fluid Pa⋅s L-1 M T-1: intensive, scalar Volume: V: Three dimensional extent of an object m 3: L 3: extensive, scalar Volumetric flow rate: Q: Rate of change of volume with respect to time m 3 ⋅s −1: L 3 T −1: extensive, scalar Wavelength: λ
From January 2008 to December 2012, if you bought shares in companies when Reuben V. Anderson joined the board, and sold them when he left, you would have a -7.1 percent return on your investment, compared to a -2.8 percent return from the S&P 500.
The Laurette T. Koellner Stock Index From June 2009 to June 2012, if you bought shares in companies when Laurette T. Koellner joined the board, and sold them when she left, you would have a 33.8 percent return on your investment, compared to a 44.2 percent return from the S&P 500.
125 psi 1.65 100 psi 1.59 80 psi 1.54 47 psi 1.38 20 psi 1.14 0 psi 0.709 List: Taylor, T.S., Elec. World, 76 (24), 1159 — 62, 1920. [32] *The report in the Data Series says that the Taylor I laminate had a thermal conductivity of 0.0996 w cm −1 K −1 at 100 psi in descent and that is an obvious typo