Eighth power

From HandWiki

In arithmetic and algebra the eighth power of a number n is the result of multiplying eight instances of n together. So:

n8 = n × n × n × n × n × n × n × n.

Eighth powers are also formed by multiplying a number by its seventh power, or the fourth power of a number by itself.

The sequence of eighth powers of integers is:

0, 1, 256, 6561, 65536, 390625, 1679616, 5764801, 16777216, 43046721, 100000000, 214358881, 429981696, 815730721, 1475789056, 2562890625, 4294967296, 6975757441, 11019960576, 16983563041, 25600000000, 37822859361, 54875873536, 78310985281, 110075314176, 152587890625 ... (sequence A001016 in the OEIS)

In the archaic notation of Robert Recorde, the eighth power of a number was called the "zenzizenzizenzic".[1]

Algebra and number theory

Polynomial equations of degree 8 are octic equations. These have the form

[math]\displaystyle{ ax^8+bx^7+cx^6+dx^5+ex^4+fx^3+gx^2+hx+k=0.\, }[/math]

The smallest known eighth power that can be written as a sum of eight eighth powers is[2]

[math]\displaystyle{ 1409^8 = 1324^8 + 1190^8 + 1088^8 + 748^8 + 524^8 + 478^8 + 223^8 + 90^8. }[/math]

The sum of the reciprocals of the nonzero eighth powers is the Riemann zeta function evaluated at 8, which can be expressed in terms of the eighth power of pi:

[math]\displaystyle{ \zeta(8) = \frac{1}{1^8} + \frac{1}{2^8} + \frac{1}{3^8} + \cdots = \frac{\pi^8}{9450} = 1.00407 \dots }[/math] (OEISA013666)

This is an example of a more general expression for evaluating the Riemann zeta function at positive even integers, in terms of the Bernoulli numbers:

[math]\displaystyle{ \zeta(2n) = (-1)^{n+1}\frac{B_{2n}(2\pi)^{2n}}{2(2n)!}. }[/math]

Physics

In aeroacoustics, Lighthill's eighth power law states that the power of the sound created by a turbulent motion, far from the turbulence, is proportional to the eighth power of the characteristic turbulent velocity.[3][4]

The ordered phase of the two-dimensional Ising model exhibits an inverse eighth power dependence of the order parameter upon the reduced temperature.[5]

The Casimir–Polder force between two molecules decays as the inverse eighth power of the distance between them.[6][7]

See also

References

  1. Womack, D. (2015), "Beyond tetration operations: their past, present and future", Mathematics in School 44 (1): 23–26, https://www.academia.edu/download/36393663/Article_4_Beyond_Tetration._accepted.doc 
  2. Quoted in Meyrignac, Jean-Charles (2001-02-14). "Computing Minimal Equal Sums Of Like Powers: Best Known Solutions". http://euler.free.fr/records.htm. 
  3. Lighthill, M. J. (1952). "On sound generated aerodynamically. I. General theory". Proc. R. Soc. Lond. A 211 (1107): 564–587. doi:10.1098/rspa.1952.0060. Bibcode1952RSPSA.211..564L. 
  4. Lighthill, M. J. (1954). "On sound generated aerodynamically. II. Turbulence as a source of sound". Proc. R. Soc. Lond. A 222 (1148): 1–32. doi:10.1098/rspa.1954.0049. Bibcode1954RSPSA.222....1L. 
  5. Kardar, Mehran (2007). Statistical Physics of Fields. Cambridge University Press. p. 148. ISBN 978-0-521-87341-3. OCLC 1026157552. https://archive.org/details/statisticalphysi00kard_650. 
  6. Casimir, H. B. G.; Polder, D. (1948). "The influence of retardation on the London-van der Waals forces". Physical Review 73 (4): 360. doi:10.1103/PhysRev.73.360. Bibcode1948PhRv...73..360C. 
  7. Derjaguin, Boris V. (1960). "The force between molecules". Scientific American 203 (1): 47–53. doi:10.1038/scientificamerican0760-47. Bibcode1960SciAm.203a..47D.