Eighth power explained

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

.

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 ...

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

ax8+bx7+cx6+dx5+ex4+fx3+gx2+hx+k=0.

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

14098=13248+11908+10888+7488+5248+4788+2238+908.

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:

\zeta(8)=

1
18

+

1
28

+

1
38

+=

\pi8
9450

=1.00407...

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:

\zeta(2n)=(-1)n+1

B2n(2\pi)2n
2(2n)!

.

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

Notes and References

  1. Womack . David . 1 . Mathematics in School . 24767659 . 23–26 . Beyond tetration operations: their past, present and future . 44 . 2015.
  2. Quoted in Web site: Meyrignac. Jean-Charles. Computing Minimal Equal Sums Of Like Powers: Best Known Solutions. 2001-02-14. 2019-12-18.
  3. Lighthill . M. J. . James Lighthill . 1952 . On sound generated aerodynamically. I. General theory . . 211 . 1107 . 564–587. 10.1098/rspa.1952.0060 . 1952RSPSA.211..564L . 124316233 .
  4. Lighthill . M. J. . James Lighthill . 1954 . On sound generated aerodynamically. II. Turbulence as a source of sound . . 222 . 1148 . 1–32. 10.1098/rspa.1954.0049 . 1954RSPSA.222....1L . 123268161 .
  5. Book: Kardar, Mehran . Mehran Kardar . Statistical Physics of Fields . limited . 148 . 2007 . Cambridge University Press . 978-0-521-87341-3 . 1026157552.
  6. Casimir . H. B. G. . Polder . D. . Hendrik Casimir . Dirk Polder . The influence of retardation on the London-van der Waals forces . . 73 . 4 . 1948 . 360 . 10.1103/PhysRev.73.360. 1948PhRv...73..360C .
  7. Derjaguin . Boris V. . Boris Derjaguin . . The force between molecules . 203 . 1 . 1960 . 47–53 . 10.1038/scientificamerican0760-47 . 2490543. 1960SciAm.203a..47D .