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PowersFractional

A power is an exponent to which a given quantity is raised. The expression x^a is therefore known as "x to the ath power." A number of powers of x are plotted above (cf. Derbyshire 2004, pp. 68 and 73).

The power may be an integer, real number, or complex number. However, the power of a real number to a non-integer power is not necessarily itself a real number. For example, x^(1/2) is real only for x>=0.

ZeroToTheZero

A number other than 0 taken to the power 0 is defined to be 1, which, for a>0, agrees with the limit

 lim_(x->0)a^x=1.
(1)

This fact is illustrated by the convergence of curves at x=0 in the plot above, which shows a^x for a=0.2, 0.4, ..., 2.0. It can also be seen more intuitively by noting that repeatedly taking the square root of a number >1 gives smaller and smaller numbers that approach one from above, while doing the same with a number between 0 and 1 gives larger and larger numbers that approach one from below. For n square roots, the total power taken is 2^(-n), which approaches 0 as n is large, giving a^0=1 in the limit that n is large.

The value of 0^0 (zero to the zeroth power) depends on the convention being used. Defining 0^0=1 allows many formulas in combinatorics to hold without exceptions. In limit calculations, however, 0^0 is an indeterminate form because the limit of f(x)^(g(x)) need not have a unique value when f(x) and g(x) both approach 0 (Knuth 1992; Knuth 1997, p. 57).

A number to the first power is, by definition, equal to itself, i.e.,

 z^1=z.
(2)

Similarly,

 1^z=1
(3)

for any complex number z. It is therefore impressive that Captain Kirk (William Shatner) is able to detect one more heartbeat aboard the starship Enterprise than can be accounted for by amplifying an auditory sensor intensified by a factor of "1 to the fourth power" in the Season 1 Star Trek episode "Court Martial" (1967).

The rules for combining quantities containing powers are called the exponent laws, and the process of raising a base to a given power is known as exponentiation.

For z!=0, with a fixed analytic branch of the complex logarithm, the derivative of z^n is given by

 d/(dz)z^n=nz^(n-1),
(4)

and the indefinite integral by

 intz^ndz={(z^(n+1))/(n+1)+C   for n!=-1; lnz+C   for n=-1.
(5)

For a real number n and 0<a<b, the definite integral is known as Cavalieri's quadrature formula and is given by

 int_a^bx^ndx={(b^(n+1)-a^(n+1))/(n+1)   for n!=-1; ln(b/a)   for n=-1.
(6)

While the simple equation

 a^x=x
(7)

for a>0 and a!=1 cannot in general be solved for x using traditional elementary functions, the solution can be given in terms of the Lambert W-function as

 x=-(W(-lna))/(lna),
(8)

where lna is the natural logarithm of a and the appropriate branch of W is chosen. For a=1, the solution is x=1.

Similarly, the solution to

 a^b=b^a
(9)

can be solved for a in terms of b using the Lambert W-function. In the special case b=2, in addition to the solutions a=2 and a=4, a third solution is

a=-(2W((ln2)/2))/(ln2)
(10)
=-0.766664696....
(11)

(OEIS A073084).

Special names given to various powers are listed in the following table.

Expressions of the form x^(x^(·^(·^·))) are known as power towers.

For integers n>=2, the largest positive integer powers p for which n=a^p with an integer a>=2 are 1, 1, 2, 1, 1, 1, 3, 2, 1, ... for n=2, 3, 4, ... (OEIS A052409). The corresponding bases a are 2, 3, 2, 5, 6, 7, 2, 3, 10, ... (OEIS A052410). For n=1, there is no finite largest exponent, since 1=1^p for every positive integer p. Sequence OEIS A052409 uses 0 at n=1 by convention.

For a positive integer n, a double binomial sum gives the power function as follows,

 sum_(k=1)^nsum_(j=1)^k(-1)^(k-j)j^n(k; j)(x; k)=x^n,
(12)

(K. MacMillan, pers. comm., Nov. 14, 2007).

For a nonnegative integer p, the power sum of the first n positive integers is given by Faulhaber's formula,

 sum_(k=1)^nk^p=1/(p+1)sum_(k=1)^(p+1)(-1)^(delta_(kp))(p+1; k)B_(p+1-k)n^k,
(13)

where delta_(kp) is the Kronecker delta, (n; k) is a binomial coefficient, and B_k is a Bernoulli number.

Let s_n be the largest integer that is not the sum of distinct nth powers of positive integers (Guy 1994). The first few values for n=2, 3, ... are 128, 12758, 5134240, 67898771, ... (OEIS A001661).

Catalan's conjecture (now a theorem) states that 8 and 9 (2^3 and 3^2) are the only consecutive perfect powers with integer bases and exponents greater than 1, i.e., the only solution to Catalan's Diophantine problem. In addition, Hyyrő and Makowski proved that there do not exist three consecutive such perfect powers (Ribenboim 1996).

Very few numbers of the form n^p+/-1 are prime (where composite powers p=kb need not be considered, since n^(kb)+/-1=(n^k)^b+/-1). The only prime numbers of the form n^p-1 for n in N and prime p correspond to n=2 and the Mersenne primes, i.e., 2^2-1=3, 2^3-1=7, 2^5-1=31, .... Other numbers of the form n^p-1 equal (n-1)×sum_(k=0)^(p-1)(n)^k. The only prime numbers of the form n^p+1 for integers n>=2 and prime p correspond to p=2 with n=2, 4, 6, 10, 14, 16, 20, 24, 26, ... (OEIS A005574, which also includes n=1). The case n=1 gives the prime 2 for every prime p. For odd prime p, n^p+1=(n+1)sum_(k=0)^(p-1)(-n)^k is composite when n>=2.

There are no nontrivial solutions to the equation

 1^n+2^n+...+m^n=(m+1)^n
(14)

for integers m, n>=2 with m<=10^(2000000) (Guy 1994, p. 153).


See also

Apocalyptic Number, Biquadratic Number, Catalan's Conjecture, Catalan's Diophantine Problem, Cavalieri's Quadrature Formula, Circle Power, Complex Exponentiation, Cube Root, Cubed, Cubic Number, Digit-Shifting Constants, Exponent, Exponent Laws, Exponential Function, Exponentiation, Faulhaber's Formula, Figurate Number, Moessner's Theorem, Narcissistic Number, Odd Power, Perfect Power, Power Rule, Power Tower, Square Number, Square Root, Squared, Sum, Truncated Power Function, Waring's Problem, Zero Explore this topic in the MathWorld classroom

Related Wolfram sites

https://functions.wolfram.com/ElementaryFunctions/Power/

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References

Barbeau, E. J. Power Play: A Country Walk through the Magical World of Numbers. Washington, DC: Math. Assoc. Amer., 1997.Beyer, W. H. "Laws of Exponents." CRC Standard Mathematical Tables, 28th ed. Boca Raton, FL: CRC Press, pp. 158 and 223, 1987.Derbyshire, J. Prime Obsession: Bernhard Riemann and the Greatest Unsolved Problem in Mathematics. New York: Penguin, 2004.Guy, R. K. "Diophantine Equations." Ch. D in Unsolved Problems in Number Theory, 2nd ed. New York: Springer-Verlag, pp. 137, 139-198, and 153-154, 1994.Knuth, D. E. "Two Notes on Notation." Amer. Math. Monthly 99, 403-422, 1992.Knuth, D. E. The Art of Computer Programming, Vol. 1: Fundamental Algorithms, 3rd ed. Reading, MA: Addison-Wesley, p. 57, 1997.Ribenboim, P. "Catalan's Conjecture." Amer. Math. Monthly 103, 529-538, 1996.Sloane, N. J. A. Sequences A001661/M5393, A005574/M1010, A052409, A052410, and A073084 in "The On-Line Encyclopedia of Integer Sequences."Spanier, J. and Oldham, K. B. "The Integer Powers (bx+c)^n and x^n" and "The Noninteger Powers x^nu." Ch. 11 and 13 in An Atlas of Functions. Washington, DC: Hemisphere, pp. 83-90 and 99-106, 1987.

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Cite this as:

Weisstein, Eric W. "Power." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/Power.html

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