Properties of the Number -94176

Ninety-Four Thousand One Hundred Seventy-Six

Basics

Value: -94177 → -94176 → -94175

Parity: even

Prime: No

Previous Prime:

Next Prime: 1

Digit Sum: 27

Digital Root: 9

Palindrome: No

Factorization: 2 ⁵ × 3 ³ × 109

Divisors: 1, 2, 3, 4, 6, 8, 9, 12, 16, 18

Polygonal

Triangular: No

Square: No

Pentagonal: No

Hexagonal: No

Heptagonal: No

Tetrahedral: No

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Representations

Binary: -10110111111100000

Octal: -267740

Duodecimal: -46600

Hexadecimal: -16fe0

Square: 8869118976

Square Root: 306.8810844610661

Classification

Fibonacci: No

Bell Number: No

Factorial Number: No

Regular Number: No

Perfect Number: No

Special

Kaprekar Constant: No

Munchausen Constant: No

Armstrong Number: No

Kaprekar Number: No

Catalan Number: No

Vampire Number: No

Taxicab Number: No

Super Prime: No

Friedman Number: No

Fermat Number: No

Cullen Number: No

OEIS Sequences

Expansion of (f(x³) / f(x))⁶ in powers of·where f() is a Ramanujan θ function. A264026

Expansion of 1/(1+2·x-2·x²+2·x³). A77984

a(n) = coefficient of xⁿ in the power series A(x) such that: 0 = ∑_{n=-oo..+oo, n<>0} n·xⁿ * (1 - xⁿ)^n-1 * A(x)ⁿ, starting with a(0) = -1. A357159

Expansion of 1/(1 - 2·x - 2·x² - 2·x³). A77835

Expansion of q^-1/2(η(q³)/η(q))⁶ in powers of q. A121596

Place two n-gons with radii 1 and 2 concentrically, forming an annular area between them. Connect all the vertices with line segments that lie entirely within that area. Then a(n) is the number of edges in that figure. A337702

Low-temperature specific heat expansion for hexagonal lattice (Potts model, q=3). A57384

Number of (1+2)X(n+2) 0..3 arrays with every 3X3 subblock row and diagonal sum equal to 0 1 3 6 or 7 and every 3X3 column and antidiagonal sum not equal to 0 1 3 6 or 7. A252306

Duplicate of A077835. A77935