fbpx
Wikipedia

Large numbers

Large numbers are numbers significantly larger than those typically used in everyday life (for instance in simple counting or in monetary transactions), appearing frequently in fields such as mathematics, cosmology, cryptography, and statistical mechanics. They are typically large positive integers, or more generally, large positive real numbers, but may also be other numbers in other contexts. Googology is the study of nomenclature and properties of large numbers.[1][2][better source needed]

In the everyday world edit

Scientific notation was created to handle the wide range of values that occur in scientific study. 1.0 × 109, for example, means one billion, or a 1 followed by nine zeros: 1 000 000 000. The reciprocal, 1.0 × 10−9, means one billionth, or 0.000 000 001. Writing 109 instead of nine zeros saves readers the effort and hazard of counting a long series of zeros to see how large the number is. In addition to scientific (powers of 10) notation, the following examples include (short scale) systematic nomenclature of large numbers.

Examples of large numbers describing everyday real-world objects include:

  • The number of cells in the human body (estimated at 3.72 × 1013), or 37.2 trillion[3]
  • The number of bits on a computer hard disk (as of 2024, typically about 1013, 1–2 TB), or 10 trillion
  • The number of neuronal connections in the human brain (estimated at 1014), or 100 trillion
  • The Avogadro constant is the number of “elementary entities” (usually atoms or molecules) in one mole; the number of atoms in 12 grams of carbon-12 – approximately 6.022×1023, or 602.2 sextillion.
  • The total number of DNA base pairs within the entire biomass on Earth, as a possible approximation of global biodiversity, is estimated at (5.3 ± 3.6) × 1037, or 53±36 undecillion[4][5]
  • The mass of Earth consists of about 4 × 1051, or 4 sexdecillion, nucleons
  • The estimated number of atoms in the observable universe (1080), or 100 quinvigintillion
  • The lower bound on the game-tree complexity of chess, also known as the “Shannon number” (estimated at around 10120), or 1 novemtrigintillion[6]

Astronomical edit

Other large numbers, as regards length and time, are found in astronomy and cosmology. For example, the current Big Bang model suggests that the universe is 13.8 billion years (4.355 × 1017 seconds) old, and that the observable universe is 93 billion light years across (8.8 × 1026 metres), and contains about 5 × 1022 stars, organized into around 125 billion (1.25 × 1011) galaxies, according to Hubble Space Telescope observations. There are about 1080 atoms in the observable universe, by rough estimation.[7]

According to Don Page, physicist at the University of Alberta, Canada, the longest finite time that has so far been explicitly calculated by any physicist is

 

which corresponds to the scale of an estimated Poincaré recurrence time for the quantum state of a hypothetical box containing a black hole with the estimated mass of the entire universe, observable or not, assuming a certain inflationary model with an inflaton whose mass is 10−6 Planck masses.[8][9] This time assumes a statistical model subject to Poincaré recurrence. A much simplified way of thinking about this time is in a model where the universe's history repeats itself arbitrarily many times due to properties of statistical mechanics; this is the time scale when it will first be somewhat similar (for a reasonable choice of "similar") to its current state again.

Combinatorial processes rapidly generate even larger numbers. The factorial function, which defines the number of permutations on a set of fixed objects, grows very rapidly with the number of objects. Stirling's formula gives a precise asymptotic expression for this rate of growth.

Combinatorial processes generate very large numbers in statistical mechanics. These numbers are so large that they are typically only referred to using their logarithms.

Gödel numbers, and similar numbers used to represent bit-strings in algorithmic information theory, are very large, even for mathematical statements of reasonable length. However, some pathological numbers are even larger than the Gödel numbers of typical mathematical propositions.

Logician Harvey Friedman has done work related to very large numbers, such as with Kruskal's tree theorem and the Robertson–Seymour theorem.

"Billions and billions" edit

To help viewers of Cosmos distinguish between "millions" and "billions", astronomer Carl Sagan stressed the "b". Sagan never did, however, say "billions and billions". The public's association of the phrase and Sagan came from a Tonight Show skit. Parodying Sagan's effect, Johnny Carson quipped "billions and billions".[10] The phrase has, however, now become a humorous fictitious number—the Sagan. Cf., Sagan Unit.

Examples edit

  • googol =  
  • centillion =   or  , depending on number naming system
  • millinillion =   or  , depending on number naming system
  • The largest known Smith number = (101031−1) × (104594 + 3×102297 + 1)1476 ×103913210
  • The largest known Mersenne prime =  [11]
  • googolplex =  
  • Skewes's numbers: the first is approximately  , the second  
  • Graham's number, larger than what can be represented even using power towers (tetration). However, it can be represented using layers of Knuth's up-arrow notation.
  • Kruskal's tree theorem is a sequence relating to graphs. TREE(3) is larger than Graham's number.
  • Rayo's number is a large number named after Agustín Rayo which has been claimed to be the largest named number. It was originally defined in a "big number duel" at MIT on 26 January 2007.

Standardized system of writing edit

A standardized way of writing very large numbers allows them to be easily sorted in increasing order, and one can get a good idea of how much larger a number is than another one.

To compare numbers in scientific notation, say 5×104 and 2×105, compare the exponents first, in this case 5 > 4, so 2×105 > 5×104. If the exponents are equal, the mantissa (or coefficient) should be compared, thus 5×104 > 2×104 because 5 > 2.

Tetration with base 10 gives the sequence  , the power towers of numbers 10, where   denotes a functional power of the function   (the function also expressed by the suffix "-plex" as in googolplex, see the googol family).

These are very round numbers, each representing an order of magnitude in a generalized sense. A crude way of specifying how large a number is, is specifying between which two numbers in this sequence it is.

More precisely, numbers in between can be expressed in the form  , i.e., with a power tower of 10s and a number at the top, possibly in scientific notation, e.g.  , a number between   and   (note that   if  ). (See also extension of tetration to real heights.)

Thus googolplex is  

Another example:

  (between   and  )

Thus the "order of magnitude" of a number (on a larger scale than usually meant), can be characterized by the number of times (n) one has to take the   to get a number between 1 and 10. Thus, the number is between   and  . As explained, a more precise description of a number also specifies the value of this number between 1 and 10, or the previous number (taking the logarithm one time less) between 10 and 1010, or the next, between 0 and 1.

Note that

 

I.e., if a number x is too large for a representation   the power tower can be made one higher, replacing x by log10x, or find x from the lower-tower representation of the log10 of the whole number. If the power tower would contain one or more numbers different from 10, the two approaches would lead to different results, corresponding to the fact that extending the power tower with a 10 at the bottom is then not the same as extending it with a 10 at the top (but, of course, similar remarks apply if the whole power tower consists of copies of the same number, different from 10).

If the height of the tower is large, the various representations for large numbers can be applied to the height itself. If the height is given only approximately, giving a value at the top does not make sense, so the double-arrow notation (e.g.  ) can be used. If the value after the double arrow is a very large number itself, the above can recursively be applied to that value.

Examples:

  (between   and  )
  (between   and  )

Similarly to the above, if the exponent of   is not exactly given then giving a value at the right does not make sense, and instead of using the power notation of  , it is possible to add   to the exponent of  , to obtain e.g.  .

If the exponent of   is large, the various representations for large numbers can be applied to this exponent itself. If this exponent is not exactly given then, again, giving a value at the right does not make sense, and instead of using the power notation of   it is possible use the triple arrow operator, e.g.  .

If the right-hand argument of the triple arrow operator is large the above applies to it, obtaining e.g.   (between   and  ). This can be done recursively, so it is possible to have a power of the triple arrow operator.

Then it is possible to proceed with operators with higher numbers of arrows, written  .

Compare this notation with the hyper operator and the Conway chained arrow notation:

  = ( abn ) = hyper(an + 2, b)

An advantage of the first is that when considered as function of b, there is a natural notation for powers of this function (just like when writing out the n arrows):  . For example:

  = ( 10 → ( 10 → ( 10 → b → 2 ) → 2 ) → 2 )

and only in special cases the long nested chain notation is reduced; for   obtains:

  = ( 10 → 3 → 3 )

Since the b can also be very large, in general it can be written instead a number with a sequence of powers   with decreasing values of n (with exactly given integer exponents  ) with at the end a number in ordinary scientific notation. Whenever a   is too large to be given exactly, the value of   is increased by 1 and everything to the right of   is rewritten.

For describing numbers approximately, deviations from the decreasing order of values of n are not needed. For example,  , and  . Thus is obtained the somewhat counterintuitive result that a number x can be so large that, in a way, x and 10x are "almost equal" (for arithmetic of large numbers see also below).

If the superscript of the upward arrow is large, the various representations for large numbers can be applied to this superscript itself. If this superscript is not exactly given then there is no point in raising the operator to a particular power or to adjust the value on which it act, instead it is possible to simply use a standard value at the right, say 10, and the expression reduces to   with an approximate n. For such numbers the advantage of using the upward arrow notation no longer applies, so the chain notation can be used instead.

The above can be applied recursively for this n, so the notation   is obtained in the superscript of the first arrow, etc., or a nested chain notation, e.g.:

(10 → 10 → (10 → 10 →  ) ) =  

If the number of levels gets too large to be convenient, a notation is used where this number of levels is written down as a number (like using the superscript of the arrow instead of writing many arrows). Introducing a function   = (10 → 10 → n), these levels become functional powers of f, allowing us to write a number in the form   where m is given exactly and n is an integer which may or may not be given exactly (for example:  ). If n is large, any of the above can be used for expressing it. The "roundest" of these numbers are those of the form fm(1) = (10→10→m→2). For example,  

Compare the definition of Graham's number: it uses numbers 3 instead of 10 and has 64 arrow levels and the number 4 at the top; thus  , but also  .

If m in   is too large to give exactly, it is possible to use a fixed n, e.g. n = 1, and apply the above recursively to m, i.e., the number of levels of upward arrows is itself represented in the superscripted upward-arrow notation, etc. Using the functional power notation of f this gives multiple levels of f. Introducing a function   these levels become functional powers of g, allowing us to write a number in the form   where m is given exactly and n is an integer which may or may not be given exactly. For example, if (10→10→m→3) = gm(1). If n is large any of the above can be used for expressing it. Similarly a function h, etc. can be introduced. If many such functions are required, they can be numbered instead of using a new letter every time, e.g. as a subscript, such that there are numbers of the form   where k and m are given exactly and n is an integer which may or may not be given exactly. Using k=1 for the f above, k=2 for g, etc., obtains (10→10→nk) =  . If n is large any of the above can be used to express it. Thus is obtained a nesting of forms   where going inward the k decreases, and with as inner argument a sequence of powers   with decreasing values of n (where all these numbers are exactly given integers) with at the end a number in ordinary scientific notation.

When k is too large to be given exactly, the number concerned can be expressed as  =(10→10→10→n) with an approximate n. Note that the process of going from the sequence  =(10→n) to the sequence  =(10→10→n) is very similar to going from the latter to the sequence  =(10→10→10→n): it is the general process of adding an element 10 to the chain in the chain notation; this process can be repeated again (see also the previous section). Numbering the subsequent versions of this function a number can be described using functions  , nested in lexicographical order with q the most significant number, but with decreasing order for q and for k; as inner argument yields a sequence of powers   with decreasing values of n (where all these numbers are exactly given integers) with at the end a number in ordinary scientific notation.

For a number too large to write down in the Conway chained arrow notation it size can be described by the length of that chain, for example only using elements 10 in the chain; in other words, one could specify its position in the sequence 10, 10→10, 10→10→10, .. If even the position in the sequence is a large number same techniques can be applied again.

Examples edit

Numbers expressible in decimal notation:

  • 22 = 4
  • 222 = 2 ↑↑ 3 = 16
  • 33 = 27
  • 44 = 256
  • 55 = 3,125
  • 66 = 46,656
  •   = 2 ↑↑ 4 = 2↑↑↑3 = 65,536
  • 77 = 823,543
  • 106 = 1,000,000 = 1 million
  • 88 = 16,777,216
  • 99 = 387,420,489
  • 109 = 1,000,000,000 = 1 billion
  • 1010 = 10,000,000,000
  • 1012 = 1,000,000,000,000 = 1 trillion
  • 333 = 3 ↑↑ 3 = 7,625,597,484,987 ≈ 7.63 × 1012
  • 1015 = 1,000,000,000,000,000 = 1 million billion = 1 quadrillion
  • 1018 = 1,000,000,000,000,000,000 = 1 billion billion = 1 quintilion

Numbers expressible in scientific notation:

  • Approximate number of atoms in the observable universe = 1080 = 100,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000
  • googol = 10100 = 10,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000,000
  • 444 = 4 ↑↑ 3 = 2512 ≈ 1.34 × 10154 ≈ (10 ↑)2 2.2
  • Approximate number of Planck volumes composing the volume of the observable universe = 8.5 × 10184
  • 555 = 5 ↑↑ 3 = 53125 ≈ 1.91 × 102184 ≈ (10 ↑)2 3.3
  •  
  • 666 = 6 ↑↑ 3 ≈ 2.66 × 1036,305 ≈ (10 ↑)2 4.6
  • 777 = 7 ↑↑ 3 ≈ 3.76 × 10695,974 ≈ (10 ↑)2 5.8
  • 888 = 8 ↑↑ 3 ≈ 6.01 × 1015,151,335 ≈ (10 ↑)2 7.2
  •  , the 51st and as of January 2021 the largest known Mersenne prime.
  • 999 = 9 ↑↑ 3 ≈ 4.28 × 10369,693,099 ≈ (10 ↑)2 8.6
  • 101010 =10 ↑↑ 3 = 1010,000,000,000 = (10 ↑)3 1
  •  

Numbers expressible in (10 ↑)n k notation:

  • googolplex =  
  •  
  •  
  •  
  •  
  • 10 ↑↑ 5 = (10 ↑)5 1
  • 3 ↑↑ 6 ≈ (10 ↑)5 1.10
  • 2 ↑↑ 8 ≈ (10 ↑)5 4.3
  • 10 ↑↑ 6 = (10 ↑)6 1
  • 10 ↑↑↑ 2 = 10 ↑↑ 10 = (10 ↑)10 1
  • 2 ↑↑↑↑ 3 = 2 ↑↑↑ 4 = 2 ↑↑ 65,536 ≈ (10 ↑)65,533 4.3 is between 10 ↑↑ 65,533 and 10 ↑↑ 65,534

Bigger numbers:

  • 3 ↑↑↑ 3 = 3 ↑↑ (3 ↑↑ 3) ≈ 3 ↑↑ 7.6 × 1012 ≈ 10 ↑↑ 7.6 × 1012 is between (10 ↑↑)2 2 and (10 ↑↑)2 3
  •   = ( 10 → 3 → 3 )
  •  
  •  
  •   = ( 10 → 4 → 3 )
  •  
  •   = ( 10 → 5 → 3 )
  •   = ( 10 → 6 → 3 )
  •   = ( 10 → 7 → 3 )
  •   = ( 10 → 8 → 3 )
  •   = ( 10 → 9 → 3 )
  •   = ( 10 → 2 → 4 ) = ( 10 → 10 → 3 )
  • The first term in the definition of Graham's number, g1 = 3 ↑↑↑↑ 3 = 3 ↑↑↑ (3 ↑↑↑ 3) ≈ 3 ↑↑↑ (10 ↑↑ 7.6 × 1012) ≈ 10 ↑↑↑ (10 ↑↑ 7.6 × 1012) is between (10 ↑↑↑)2 2 and (10 ↑↑↑)2 3 (See Graham's number#Magnitude)
  •   = (10 → 3 → 4)
  •   = ( 4 → 4 → 4 )  
  •   = ( 10 → 4 → 4 )
  •   = ( 10 → 5 → 4 )
  •   = ( 10 → 6 → 4 )
  •   = ( 10 → 7 → 4 )
  •   = ( 10 → 8 → 4 )
  •   = ( 10 → 9 → 4 )
  •   = ( 10 → 2 → 5 ) = ( 10 → 10 → 4 )
  • ( 2 → 3 → 2 → 2 ) = ( 2 → 3 → 8 )
  • ( 3 → 2 → 2 → 2 ) = ( 3 → 2 → 9 ) = ( 3 → 3 → 8 )
  • ( 10 → 10 → 10 ) = ( 10 → 2 → 11 )
  • ( 10 → 2 → 2 → 2 ) = ( 10 → 2 → 100 )
  • ( 10 → 10 → 2 → 2 ) = ( 10 → 2 →   ) =  
  • The second term in the definition of Graham's number, g2 = 3 ↑g1 3 > 10 ↑g1 – 1 10.
  • ( 10 → 10 → 3 → 2 ) = (10 → 10 → (10 → 10 →  ) ) =  
  • g3 = (3 → 3 → g2) > (10 → 10 → g2 – 1) > (10 → 10 → 3 → 2)
  • g4 = (3 → 3 → g3) > (10 → 10 → g3 – 1) > (10 → 10 → 4 → 2)
  • ...
  • g9 = (3 → 3 → g8) is between (10 → 10 → 9 → 2) and (10 → 10 → 10 → 2)
  • ( 10 → 10 → 10 → 2 )
  • g10 = (3 → 3 → g9) is between (10 → 10 → 10 → 2) and (10 → 10 → 11 → 2)
  • ...
  • g63 = (3 → 3 → g62) is between (10 → 10 → 63 → 2) and (10 → 10 → 64 → 2)
  • ( 10 → 10 → 64 → 2 )
  • Graham's number, g64[12]
  • ( 10 → 10 → 65 → 2 )
  • ( 10 → 10 → 10 → 3 )
  • ( 10 → 10 → 10 → 4 )
  • ( 10 → 10 → 10 → 10 )
  • ( 10 → 10 → 10 → 10 → 10 )
  • ( 10 → 10 → 10 → 10 → 10 → 10 )
  • ( 10 → 10 → 10 → 10 → 10 → 10 → 10 → ... → 10 → 10 → 10 → 10 → 10 → 10 → 10 → 10 ) where there are ( 10 → 10 → 10 ) "10"s

Other notations edit

Some notations for extremely large numbers:

These notations are essentially functions of integer variables, which increase very rapidly with those integers. Ever-faster-increasing functions can easily be constructed recursively by applying these functions with large integers as argument.

A function with a vertical asymptote is not helpful in defining a very large number, although the function increases very rapidly: one has to define an argument very close to the asymptote, i.e. use a very small number, and constructing that is equivalent to constructing a very large number, e.g. the reciprocal.

Comparison of base values edit

The following illustrates the effect of a base different from 10, base 100. It also illustrates representations of numbers and the arithmetic.

 , with base 10 the exponent is doubled.

 , ditto.

 , the highest exponent is very little more than doubled (increased by log102).

  •  
  •  
  •  
  •   (thus if n is large it seems fair to say that   is "approximately equal to"  )
  •  
  •  
  •   (compare  ; thus if n is large it seems fair to say that   is "approximately equal to"  )
  •   (compare  )
  •   (compare  )
  •   (compare  ; if n is large this is "approximately" equal)

Accuracy edit

For a number  , one unit change in n changes the result by a factor 10. In a number like  , with the 6.2 the result of proper rounding using significant figures, the true value of the exponent may be 50 less or 50 more. Hence the result may be a factor   too large or too small. This seems like extremely poor accuracy, but for such a large number it may be considered fair (a large error in a large number may be "relatively small" and therefore acceptable).

For very large numbers edit

In the case of an approximation of an extremely large number, the relative error may be large, yet there may still be a sense in which one wants to consider the numbers as "close in magnitude". For example, consider

  and  

The relative error is

 

a large relative error. However, one can also consider the relative error in the logarithms; in this case, the logarithms (to base 10) are 10 and 9, so the relative error in the logarithms is only 10%.

The point is that exponential functions magnify relative errors greatly – if a and b have a small relative error,

  and  

the relative error is larger, and

  and  

will have an even larger relative error. The question then becomes: on which level of iterated logarithms do to compare two numbers? There is a sense in which one may want to consider

  and  

to be "close in magnitude". The relative error between these two numbers is large, and the relative error between their logarithms is still large; however, the relative error in their second-iterated logarithms is small:

  and  

Such comparisons of iterated logarithms are common, e.g., in analytic number theory.

Classes edit

One solution to the problem of comparing large numbers is to define classes of numbers, such as the system devised by Robert Munafo,[13] which is based on different "levels" of perception of an average person. Class 0 – numbers between zero and six – is defined to contain numbers that are easily subitized, that is, numbers that show up very frequently in daily life and are almost instantly comparable. Class 1 – numbers between six and 1,000,000=106 – is defined to contain numbers whose decimal expressions are easily subitized, that is, numbers who are easily comparable not by cardinality, but "at a glance" given the decimal expansion.

Each class after these are defined in terms of iterating this base-10 exponentiation, to simulate the effect of another "iteration" of human indistinguishibility. For example, class 5 is defined to include numbers between 101010106 and 10101010106, which are numbers where X becomes humanly indistinguishable from X2 [14] (taking iterated logarithms of such X yields indistinguishibility firstly between log(X) and 2log(X), secondly between log(log(X)) and 1+log(log(X)), and finally an extremely long decimal expansion whose length can't be subitized).

Approximate arithmetic edit

There are some general rules relating to the usual arithmetic operations performed on very large numbers:

  • The sum and the product of two very large numbers are both "approximately" equal to the larger one.
  •  

Hence:

  • A very large number raised to a very large power is "approximately" equal to the larger of the following two values: the first value and 10 to the power the second. For example, for very large   there is   (see e.g. the computation of mega) and also  . Thus  , see table.

Systematically creating ever-faster-increasing sequences edit

Given a strictly increasing integer sequence/function   (n≥1), it is possible to produce a faster-growing sequence   (where the superscript n denotes the nth functional power). This can be repeated any number of times by letting  , each sequence growing much faster than the one before it. Thus it is possible to define  , which grows much faster than any   for finite k (here ω is the first infinite ordinal number, representing the limit of all finite numbers k). This is the basis for the fast-growing hierarchy of functions, in which the indexing subscript is extended to ever-larger ordinals.

For example, starting with f0(n) = n + 1:

  • f1(n) = f0n(n) = n + n = 2n
  • f2(n) = f1n(n) = 2nn > (2 ↑) n for n ≥ 2 (using Knuth up-arrow notation)
  • f3(n) = f2n(n) > (2 ↑)n n ≥ 2 ↑2 n for n ≥ 2
  • fk+1(n) > 2 ↑k n for n ≥ 2, k < ω
  • fω(n) = fn(n) > 2 ↑n – 1 n > 2 ↑n − 2 (n + 3) − 3 = A(n, n) for n ≥ 2, where A is the Ackermann function (of which fω is a unary version)
  • fω+1(64) > fω64(6) > Graham's number (= g64 in the sequence defined by g0 = 4, gk+1 = 3 ↑gk 3)
    • This follows by noting fω(n) > 2 ↑n – 1 n > 3 ↑n – 2 3 + 2, and hence fω(gk + 2) > gk+1 + 2
  • fω(n) > 2 ↑n – 1 n = (2 → nn-1) = (2 → nn-1 → 1) (using Conway chained arrow notation)
  • fω+1(n) = fωn(n) > (2 → nn-1 → 2) (because if gk(n) = X → nk then X → nk+1 = gkn(1))
  • fω+k(n) > (2 → nn-1 → k+1) > (nnk)
  • fω2(n) = fω+n(n) > (nnn) = (nnn→ 1)
  • fω2+k(n) > (nnnk)
  • fω3(n) > (nnnn)
  • fωk(n) > (nn → ... → nn) (Chain of k+1 n's)
  • fω2(n) = fωn(n) > (nn → ... → nn) (Chain of n+1 n's)

In some noncomputable sequences edit

The busy beaver function Σ is an example of a function which grows faster than any computable function. Its value for even relatively small input is huge. The values of Σ(n) for n = 1, 2, 3, 4 are 1, 4, 6, 13 (sequence A028444 in the OEIS). Σ(5) is not known but is definitely ≥ 4098. Σ(6) is at least 10↑↑15.

Infinite numbers edit

Although all the numbers discussed above are very large, they are all still decidedly finite. Certain fields of mathematics define infinite and transfinite numbers. For example, aleph-null is the cardinality of the infinite set of natural numbers, and aleph-one is the next greatest cardinal number.   is the cardinality of the reals. The proposition that   is known as the continuum hypothesis.

See also edit

References edit

  1. ^ One Million Things: A Visual Encyclopedia[unreliable source?]
  2. ^ «The study of large numbers is called googology»[unreliable source?]
  3. ^ Bianconi, Eva; Piovesan, Allison; Facchin, Federica; Beraudi, Alina; Casadei, Raffaella; Frabetti, Flavia; Vitale, Lorenza; Pelleri, Maria Chiara; Tassani, Simone (Nov–Dec 2013). "An estimation of the number of cells in the human body". Annals of Human Biology. 40 (6): 463–471. doi:10.3109/03014460.2013.807878. hdl:11585/152451. ISSN 1464-5033. PMID 23829164. S2CID 16247166.
  4. ^ Landenmark HK, Forgan DH, Cockell CS (June 2015). "An Estimate of the Total DNA in the Biosphere". PLOS Biology. 13 (6): e1002168. doi:10.1371/journal.pbio.1002168. PMC 4466264. PMID 26066900.
  5. ^ Nuwer R (18 July 2015). "Counting All the DNA on Earth". The New York Times. New York. ISSN 0362-4331. Retrieved 2015-07-18.
  6. ^ Shannon, Claude (March 1950). (PDF). Philosophical Magazine. Series 7. 41 (314). Archived from the original (PDF) on 2010-07-06. Retrieved 2019-01-25.
  7. ^ Atoms in the Universe. Universe Today. 30-07-2009. Retrieved 02-03-13.
  8. ^ Information Loss in Black Holes and/or Conscious Beings?, Don N. Page, Heat Kernel Techniques and Quantum Gravity (1995), S. A. Fulling (ed), p. 461. Discourses in Mathematics and its Applications, No. 4, Texas A&M University Department of Mathematics. arXiv:hep-th/9411193. ISBN 0-9630728-3-8.
  9. ^ How to Get A Googolplex
  10. ^ Carl Sagan takes questions more from his 'Wonder and Skepticism' CSICOP 1994 keynote, Skeptical Inquirer December 21, 2016, at the Wayback Machine
  11. ^ "GIMPS Discovers Largest Known Prime Number". Great Internet Mersenne Prime Search. 2018-12-21.
  12. ^ Regarding the comparison with the previous value:  , so starting the 64 steps with 1 instead of 4 more than compensates for replacing the numbers 3 by 10
  13. ^ "Large Numbers at MROB". www.mrob.com. Retrieved 2021-05-13.
  14. ^ "Large Numbers (page 2) at MROB". www.mrob.com. Retrieved 2021-05-13.

large, numbers, other, uses, large, number, disambiguation, numbers, significantly, larger, than, those, typically, used, everyday, life, instance, simple, counting, monetary, transactions, appearing, frequently, fields, such, mathematics, cosmology, cryptogra. For other uses see Large number disambiguation Large numbers are numbers significantly larger than those typically used in everyday life for instance in simple counting or in monetary transactions appearing frequently in fields such as mathematics cosmology cryptography and statistical mechanics They are typically large positive integers or more generally large positive real numbers but may also be other numbers in other contexts Googology is the study of nomenclature and properties of large numbers 1 2 better source needed Contents 1 In the everyday world 2 Astronomical 2 1 Billions and billions 3 Examples 4 Standardized system of writing 4 1 Examples 4 2 Other notations 5 Comparison of base values 6 Accuracy 6 1 For very large numbers 6 2 Classes 6 3 Approximate arithmetic 7 Systematically creating ever faster increasing sequences 8 In some noncomputable sequences 9 Infinite numbers 10 See also 11 ReferencesIn the everyday world editSee also Scientific notation Logarithmic scale Orders of magnitude and Names of large numbers Scientific notation was created to handle the wide range of values that occur in scientific study 1 0 109 for example means one billion or a 1 followed by nine zeros 1 000 000 000 The reciprocal 1 0 10 9 means one billionth or 0 000 000 001 Writing 109 instead of nine zeros saves readers the effort and hazard of counting a long series of zeros to see how large the number is In addition to scientific powers of 10 notation the following examples include short scale systematic nomenclature of large numbers Examples of large numbers describing everyday real world objects include The number of cells in the human body estimated at 3 72 1013 or 37 2 trillion 3 The number of bits on a computer hard disk as of 2024 update typically about 1013 1 2 TB or 10 trillion The number of neuronal connections in the human brain estimated at 1014 or 100 trillion The Avogadro constant is the number of elementary entities usually atoms or molecules in one mole the number of atoms in 12 grams of carbon 12 approximately 6 022 1023 or 602 2 sextillion The total number of DNA base pairs within the entire biomass on Earth as a possible approximation of global biodiversity is estimated at 5 3 3 6 1037 or 53 36 undecillion 4 5 The mass of Earth consists of about 4 1051 or 4 sexdecillion nucleons The estimated number of atoms in the observable universe 1080 or 100 quinvigintillion The lower bound on the game tree complexity of chess also known as the Shannon number estimated at around 10120 or 1 novemtrigintillion 6 Note that this value of the Shannon number is for Standard Chess It has even larger values for larger board chess variants such as Grant Acedrex Tai Shogi and Taikyoku Shogi Astronomical editOther large numbers as regards length and time are found in astronomy and cosmology For example the current Big Bang model suggests that the universe is 13 8 billion years 4 355 1017 seconds old and that the observable universe is 93 billion light years across 8 8 1026 metres and contains about 5 1022 stars organized into around 125 billion 1 25 1011 galaxies according to Hubble Space Telescope observations There are about 1080 atoms in the observable universe by rough estimation 7 According to Don Page physicist at the University of Alberta Canada the longest finite time that has so far been explicitly calculated by any physicist is 10 10 10 10 10 1 1 years displaystyle 10 10 10 10 10 1 1 mbox years nbsp dd dd dd which corresponds to the scale of an estimated Poincare recurrence time for the quantum state of a hypothetical box containing a black hole with the estimated mass of the entire universe observable or not assuming a certain inflationary model with an inflaton whose mass is 10 6 Planck masses 8 9 This time assumes a statistical model subject to Poincare recurrence A much simplified way of thinking about this time is in a model where the universe s history repeats itself arbitrarily many times due to properties of statistical mechanics this is the time scale when it will first be somewhat similar for a reasonable choice of similar to its current state again Combinatorial processes rapidly generate even larger numbers The factorial function which defines the number of permutations on a set of fixed objects grows very rapidly with the number of objects Stirling s formula gives a precise asymptotic expression for this rate of growth Combinatorial processes generate very large numbers in statistical mechanics These numbers are so large that they are typically only referred to using their logarithms Godel numbers and similar numbers used to represent bit strings in algorithmic information theory are very large even for mathematical statements of reasonable length However some pathological numbers are even larger than the Godel numbers of typical mathematical propositions Logician Harvey Friedman has done work related to very large numbers such as with Kruskal s tree theorem and the Robertson Seymour theorem Billions and billions edit To help viewers of Cosmos distinguish between millions and billions astronomer Carl Sagan stressed the b Sagan never did however say billions and billions The public s association of the phrase and Sagan came from a Tonight Show skit Parodying Sagan s effect Johnny Carson quipped billions and billions 10 The phrase has however now become a humorous fictitious number the Sagan Cf Sagan Unit Examples editgoogol 10 100 displaystyle 10 100 nbsp centillion 10 303 displaystyle 10 303 nbsp or 10 600 displaystyle 10 600 nbsp depending on number naming system millinillion 10 3003 displaystyle 10 3003 nbsp or 10 6000 displaystyle 10 6000 nbsp depending on number naming system The largest known Smith number 101031 1 104594 3 102297 1 1476 103913 210 The largest known Mersenne prime 2 82 589 933 1 displaystyle 2 82 589 933 1 nbsp 11 googolplex 10 googol 10 10 100 displaystyle 10 text googol 10 10 100 nbsp Skewes s numbers the first is approximately 10 10 10 34 displaystyle 10 10 10 34 nbsp the second 10 10 10 964 displaystyle 10 10 10 964 nbsp Graham s number larger than what can be represented even using power towers tetration However it can be represented using layers of Knuth s up arrow notation Kruskal s tree theorem is a sequence relating to graphs TREE 3 is larger than Graham s number Rayo s number is a large number named after Agustin Rayo which has been claimed to be the largest named number It was originally defined in a big number duel at MIT on 26 January 2007 Standardized system of writing editThis section does not cite any sources Please help improve this section by adding citations to reliable sources Unsourced material may be challenged and removed December 2022 Learn how and when to remove this message A standardized way of writing very large numbers allows them to be easily sorted in increasing order and one can get a good idea of how much larger a number is than another one To compare numbers in scientific notation say 5 104 and 2 105 compare the exponents first in this case 5 gt 4 so 2 105 gt 5 104 If the exponents are equal the mantissa or coefficient should be compared thus 5 104 gt 2 104 because 5 gt 2 Tetration with base 10 gives the sequence 10 n 10 n 2 10 n 1 displaystyle 10 uparrow uparrow n 10 to n to 2 10 uparrow n 1 nbsp the power towers of numbers 10 where 10 n displaystyle 10 uparrow n nbsp denotes a functional power of the function f n 10 n displaystyle f n 10 n nbsp the function also expressed by the suffix plex as in googolplex see the googol family These are very round numbers each representing an order of magnitude in a generalized sense A crude way of specifying how large a number is is specifying between which two numbers in this sequence it is More precisely numbers in between can be expressed in the form 10 n a displaystyle 10 uparrow n a nbsp i e with a power tower of 10s and a number at the top possibly in scientific notation e g 10 10 10 10 10 4 829 10 5 4 829 displaystyle 10 10 10 10 10 4 829 10 uparrow 5 4 829 nbsp a number between 10 5 displaystyle 10 uparrow uparrow 5 nbsp and 10 6 displaystyle 10 uparrow uparrow 6 nbsp note that 10 n lt 10 n a lt 10 n 1 displaystyle 10 uparrow uparrow n lt 10 uparrow n a lt 10 uparrow uparrow n 1 nbsp if 1 lt a lt 10 displaystyle 1 lt a lt 10 nbsp See also extension of tetration to real heights Thus googolplex is 10 10 100 10 2 100 10 3 2 displaystyle 10 10 100 10 uparrow 2 100 10 uparrow 3 2 nbsp Another example 2 4 2 2 2 65 536 copies of 2 10 65 531 6 10 19 728 10 65 533 4 3 displaystyle 2 uparrow uparrow uparrow 4 begin matrix underbrace 2 2 2 qquad quad 65 536 mbox copies of 2 end matrix approx 10 uparrow 65 531 6 times 10 19 728 approx 10 uparrow 65 533 4 3 nbsp between 10 65 533 displaystyle 10 uparrow uparrow 65 533 nbsp and 10 65 534 displaystyle 10 uparrow uparrow 65 534 nbsp Thus the order of magnitude of a number on a larger scale than usually meant can be characterized by the number of times n one has to take the l o g 10 displaystyle log 10 nbsp to get a number between 1 and 10 Thus the number is between 10 n displaystyle 10 uparrow uparrow n nbsp and 10 n 1 displaystyle 10 uparrow uparrow n 1 nbsp As explained a more precise description of a number also specifies the value of this number between 1 and 10 or the previous number taking the logarithm one time less between 10 and 1010 or the next between 0 and 1 Note that 10 10 n x 10 n 10 x displaystyle 10 10 uparrow n x 10 uparrow n 10 x nbsp I e if a number x is too large for a representation 10 n x displaystyle 10 uparrow n x nbsp the power tower can be made one higher replacing x by log10x or find x from the lower tower representation of the log10 of the whole number If the power tower would contain one or more numbers different from 10 the two approaches would lead to different results corresponding to the fact that extending the power tower with a 10 at the bottom is then not the same as extending it with a 10 at the top but of course similar remarks apply if the whole power tower consists of copies of the same number different from 10 If the height of the tower is large the various representations for large numbers can be applied to the height itself If the height is given only approximately giving a value at the top does not make sense so the double arrow notation e g 10 7 21 10 8 displaystyle 10 uparrow uparrow 7 21 times 10 8 nbsp can be used If the value after the double arrow is a very large number itself the above can recursively be applied to that value Examples 10 10 10 10 3 81 10 17 displaystyle 10 uparrow uparrow 10 10 10 3 81 times 10 17 nbsp between 10 2 displaystyle 10 uparrow uparrow uparrow 2 nbsp and 10 3 displaystyle 10 uparrow uparrow uparrow 3 nbsp 10 10 10 497 9 73 10 32 10 2 10 497 9 73 10 32 displaystyle 10 uparrow uparrow 10 uparrow uparrow 10 uparrow 497 9 73 times 10 32 10 uparrow uparrow 2 10 uparrow 497 9 73 times 10 32 nbsp between 10 4 displaystyle 10 uparrow uparrow uparrow 4 nbsp and 10 5 displaystyle 10 uparrow uparrow uparrow 5 nbsp Similarly to the above if the exponent of 10 displaystyle 10 uparrow nbsp is not exactly given then giving a value at the right does not make sense and instead of using the power notation of 10 displaystyle 10 uparrow nbsp it is possible to add 1 displaystyle 1 nbsp to the exponent of 10 displaystyle 10 uparrow uparrow nbsp to obtain e g 10 3 2 8 10 12 displaystyle 10 uparrow uparrow 3 2 8 times 10 12 nbsp If the exponent of 10 displaystyle 10 uparrow uparrow nbsp is large the various representations for large numbers can be applied to this exponent itself If this exponent is not exactly given then again giving a value at the right does not make sense and instead of using the power notation of 10 displaystyle 10 uparrow uparrow nbsp it is possible use the triple arrow operator e g 10 7 3 10 6 displaystyle 10 uparrow uparrow uparrow 7 3 times 10 6 nbsp If the right hand argument of the triple arrow operator is large the above applies to it obtaining e g 10 10 2 10 497 9 73 10 32 displaystyle 10 uparrow uparrow uparrow 10 uparrow uparrow 2 10 uparrow 497 9 73 times 10 32 nbsp between 10 10 4 displaystyle 10 uparrow uparrow uparrow 10 uparrow uparrow uparrow 4 nbsp and 10 10 5 displaystyle 10 uparrow uparrow uparrow 10 uparrow uparrow uparrow 5 nbsp This can be done recursively so it is possible to have a power of the triple arrow operator Then it is possible to proceed with operators with higher numbers of arrows written n displaystyle uparrow n nbsp Compare this notation with the hyper operator and the Conway chained arrow notation a n b displaystyle a uparrow n b nbsp a b n hyper a n 2 b An advantage of the first is that when considered as function of b there is a natural notation for powers of this function just like when writing out the n arrows a n k b displaystyle a uparrow n k b nbsp For example 10 2 3 b displaystyle 10 uparrow 2 3 b nbsp 10 10 10 b 2 2 2 and only in special cases the long nested chain notation is reduced for b 1 displaystyle b 1 nbsp obtains 10 3 3 10 2 3 1 displaystyle 10 uparrow 3 3 10 uparrow 2 3 1 nbsp 10 3 3 Since the b can also be very large in general it can be written instead a number with a sequence of powers 10 n k n displaystyle 10 uparrow n k n nbsp with decreasing values of n with exactly given integer exponents k n displaystyle k n nbsp with at the end a number in ordinary scientific notation Whenever a k n displaystyle k n nbsp is too large to be given exactly the value of k n 1 displaystyle k n 1 nbsp is increased by 1 and everything to the right of n 1 k n 1 displaystyle n 1 k n 1 nbsp is rewritten For describing numbers approximately deviations from the decreasing order of values of n are not needed For example 10 10 5 a 10 6 a displaystyle 10 uparrow 10 uparrow uparrow 5 a 10 uparrow uparrow 6 a nbsp and 10 10 3 10 10 10 1 10 3 displaystyle 10 uparrow 10 uparrow uparrow uparrow 3 10 uparrow uparrow 10 uparrow uparrow 10 1 approx 10 uparrow uparrow uparrow 3 nbsp Thus is obtained the somewhat counterintuitive result that a number x can be so large that in a way x and 10x are almost equal for arithmetic of large numbers see also below If the superscript of the upward arrow is large the various representations for large numbers can be applied to this superscript itself If this superscript is not exactly given then there is no point in raising the operator to a particular power or to adjust the value on which it act instead it is possible to simply use a standard value at the right say 10 and the expression reduces to 10 n 10 10 10 n displaystyle 10 uparrow n 10 10 to 10 to n nbsp with an approximate n For such numbers the advantage of using the upward arrow notation no longer applies so the chain notation can be used instead The above can be applied recursively for this n so the notation n displaystyle uparrow n nbsp is obtained in the superscript of the first arrow etc or a nested chain notation e g 10 10 10 10 3 10 5 displaystyle 3 times 10 5 nbsp 10 10 3 10 5 10 10 displaystyle 10 uparrow 10 uparrow 3 times 10 5 10 10 nbsp If the number of levels gets too large to be convenient a notation is used where this number of levels is written down as a number like using the superscript of the arrow instead of writing many arrows Introducing a function f n 10 n 10 displaystyle f n 10 uparrow n 10 nbsp 10 10 n these levels become functional powers of f allowing us to write a number in the form f m n displaystyle f m n nbsp where m is given exactly and n is an integer which may or may not be given exactly for example f 2 3 10 5 displaystyle f 2 3 times 10 5 nbsp If n is large any of the above can be used for expressing it The roundest of these numbers are those of the form fm 1 10 10 m 2 For example 10 10 3 2 10 10 10 10 10 10 displaystyle 10 to 10 to 3 to 2 10 uparrow 10 uparrow 10 10 10 10 nbsp Compare the definition of Graham s number it uses numbers 3 instead of 10 and has 64 arrow levels and the number 4 at the top thus G lt 3 3 65 2 lt 10 10 65 2 f 65 1 displaystyle G lt 3 rightarrow 3 rightarrow 65 rightarrow 2 lt 10 to 10 to 65 to 2 f 65 1 nbsp but also G lt f 64 4 lt f 65 1 displaystyle G lt f 64 4 lt f 65 1 nbsp If m in f m n displaystyle f m n nbsp is too large to give exactly it is possible to use a fixed n e g n 1 and apply the above recursively to m i e the number of levels of upward arrows is itself represented in the superscripted upward arrow notation etc Using the functional power notation of f this gives multiple levels of f Introducing a function g n f n 1 displaystyle g n f n 1 nbsp these levels become functional powers of g allowing us to write a number in the form g m n displaystyle g m n nbsp where m is given exactly and n is an integer which may or may not be given exactly For example if 10 10 m 3 gm 1 If n is large any of the above can be used for expressing it Similarly a function h etc can be introduced If many such functions are required they can be numbered instead of using a new letter every time e g as a subscript such that there are numbers of the form f k m n displaystyle f k m n nbsp where k and m are given exactly and n is an integer which may or may not be given exactly Using k 1 for the f above k 2 for g etc obtains 10 10 n k f k n f k 1 n 1 displaystyle f k n f k 1 n 1 nbsp If n is large any of the above can be used to express it Thus is obtained a nesting of forms f k m k displaystyle f k m k nbsp where going inward the k decreases and with as inner argument a sequence of powers 10 n p n displaystyle 10 uparrow n p n nbsp with decreasing values of n where all these numbers are exactly given integers with at the end a number in ordinary scientific notation When k is too large to be given exactly the number concerned can be expressed as f n 10 displaystyle f n 10 nbsp 10 10 10 n with an approximate n Note that the process of going from the sequence 10 n displaystyle 10 n nbsp 10 n to the sequence 10 n 10 displaystyle 10 uparrow n 10 nbsp 10 10 n is very similar to going from the latter to the sequence f n 10 displaystyle f n 10 nbsp 10 10 10 n it is the general process of adding an element 10 to the chain in the chain notation this process can be repeated again see also the previous section Numbering the subsequent versions of this function a number can be described using functions f q k m q k displaystyle f qk m qk nbsp nested in lexicographical order with q the most significant number but with decreasing order for q and for k as inner argument yields a sequence of powers 10 n p n displaystyle 10 uparrow n p n nbsp with decreasing values of n where all these numbers are exactly given integers with at the end a number in ordinary scientific notation For a number too large to write down in the Conway chained arrow notation it size can be described by the length of that chain for example only using elements 10 in the chain in other words one could specify its position in the sequence 10 10 10 10 10 10 If even the position in the sequence is a large number same techniques can be applied again Examples edit Numbers expressible in decimal notation 22 4 222 2 3 16 33 27 44 256 55 3 125 66 46 656 2 2 2 2 displaystyle 2 2 2 2 nbsp 2 4 2 3 65 536 77 823 543 106 1 000 000 1 million 88 16 777 216 99 387 420 489 109 1 000 000 000 1 billion 1010 10 000 000 000 1012 1 000 000 000 000 1 trillion 333 3 3 7 625 597 484 987 7 63 1012 1015 1 000 000 000 000 000 1 million billion 1 quadrillion 1018 1 000 000 000 000 000 000 1 billion billion 1 quintilion Numbers expressible in scientific notation Approximate number of atoms in the observable universe 1080 100 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 googol 10100 10 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 000 444 4 3 2512 1 34 10154 10 2 2 2 Approximate number of Planck volumes composing the volume of the observable universe 8 5 10184 555 5 3 53125 1 91 102184 10 2 3 3 2 2 2 2 2 2 5 2 65 536 2 0 10 19 728 10 2 4 3 displaystyle 2 2 2 2 2 2 uparrow uparrow 5 2 65 536 approx 2 0 times 10 19 728 approx 10 uparrow 2 4 3 nbsp 666 6 3 2 66 1036 305 10 2 4 6 777 7 3 3 76 10695 974 10 2 5 8 888 8 3 6 01 1015 151 335 10 2 7 2 M 82 589 933 1 49 10 24 862 047 10 10 7 3955 10 2 7 3955 displaystyle M 82 589 933 approx 1 49 times 10 24 862 047 approx 10 10 7 3955 10 uparrow 2 7 3955 nbsp the 51st and as of January 2021 update the largest known Mersenne prime 999 9 3 4 28 10369 693 099 10 2 8 6 101010 10 3 1010 000 000 000 10 3 1 3 3 3 3 3 4 1 26 10 3 638 334 640 024 10 3 1 10 displaystyle 3 3 3 3 3 uparrow uparrow 4 approx 1 26 times 10 3 638 334 640 024 approx 10 uparrow 3 1 10 nbsp Numbers expressible in 10 n k notation googolplex 10 10 100 10 3 2 displaystyle 10 10 100 10 uparrow 3 2 nbsp 2 2 2 2 2 2 2 6 2 2 65 536 2 10 2 4 3 10 10 2 4 3 10 3 4 3 displaystyle 2 2 2 2 2 2 2 uparrow uparrow 6 2 2 65 536 approx 2 10 uparrow 2 4 3 approx 10 10 uparrow 2 4 3 10 uparrow 3 4 3 nbsp 10 10 10 10 10 4 10 4 1 displaystyle 10 10 10 10 10 uparrow uparrow 4 10 uparrow 4 1 nbsp 3 3 3 3 3 3 5 3 10 3 6 10 12 10 4 1 10 displaystyle 3 3 3 3 3 3 uparrow uparrow 5 approx 3 10 3 6 times 10 12 approx 10 uparrow 4 1 10 nbsp 2 2 2 2 2 2 2 2 7 10 4 4 3 displaystyle 2 2 2 2 2 2 2 2 uparrow uparrow 7 approx 10 uparrow 4 4 3 nbsp 10 5 10 5 1 3 6 10 5 1 10 2 8 10 5 4 3 10 6 10 6 1 10 2 10 10 10 10 1 2 3 2 4 2 65 536 10 65 533 4 3 is between 10 65 533 and 10 65 534 Bigger numbers 3 3 3 3 3 3 7 6 1012 10 7 6 1012 is between 10 2 2 and 10 2 3 10 3 10 3 1 displaystyle 10 uparrow uparrow uparrow 3 10 uparrow uparrow 3 1 nbsp 10 3 3 10 2 11 displaystyle 10 uparrow uparrow 2 11 nbsp 10 2 10 10 10 3 81 10 17 displaystyle 10 uparrow uparrow 2 10 10 10 3 81 times 10 17 nbsp 10 4 10 4 1 displaystyle 10 uparrow uparrow uparrow 4 10 uparrow uparrow 4 1 nbsp 10 4 3 10 2 10 497 9 73 10 32 displaystyle 10 uparrow uparrow 2 10 uparrow 497 9 73 times 10 32 nbsp 10 5 10 5 1 displaystyle 10 uparrow uparrow uparrow 5 10 uparrow uparrow 5 1 nbsp 10 5 3 10 6 10 6 1 displaystyle 10 uparrow uparrow uparrow 6 10 uparrow uparrow 6 1 nbsp 10 6 3 10 7 10 7 1 displaystyle 10 uparrow uparrow uparrow 7 10 uparrow uparrow 7 1 nbsp 10 7 3 10 8 10 8 1 displaystyle 10 uparrow uparrow uparrow 8 10 uparrow uparrow 8 1 nbsp 10 8 3 10 9 10 9 1 displaystyle 10 uparrow uparrow uparrow 9 10 uparrow uparrow 9 1 nbsp 10 9 3 10 2 10 10 10 10 1 displaystyle 10 uparrow uparrow uparrow uparrow 2 10 uparrow uparrow uparrow 10 10 uparrow uparrow 10 1 nbsp 10 2 4 10 10 3 The first term in the definition of Graham s number g1 3 3 3 3 3 3 10 7 6 1012 10 10 7 6 1012 is between 10 2 2 and 10 2 3 See Graham s number Magnitude 10 3 10 3 1 displaystyle 10 uparrow uparrow uparrow uparrow 3 10 uparrow uparrow uparrow 3 1 nbsp 10 3 4 4 4 displaystyle 4 uparrow uparrow uparrow uparrow 4 nbsp 4 4 4 10 2 10 3 154 displaystyle approx 10 uparrow uparrow uparrow 2 10 uparrow uparrow 3 154 nbsp 10 4 10 4 1 displaystyle 10 uparrow uparrow uparrow uparrow 4 10 uparrow uparrow uparrow 4 1 nbsp 10 4 4 10 5 10 5 1 displaystyle 10 uparrow uparrow uparrow uparrow 5 10 uparrow uparrow uparrow 5 1 nbsp 10 5 4 10 6 10 6 1 displaystyle 10 uparrow uparrow uparrow uparrow 6 10 uparrow uparrow uparrow 6 1 nbsp 10 6 4 10 7 10 7 1 displaystyle 10 uparrow uparrow uparrow uparrow 7 10 uparrow uparrow uparrow 7 1 nbsp 10 7 4 10 8 10 8 1 displaystyle 10 uparrow uparrow uparrow uparrow 8 10 uparrow uparrow uparrow 8 1 nbsp 10 8 4 10 9 10 9 1 displaystyle 10 uparrow uparrow uparrow uparrow 9 10 uparrow uparrow uparrow 9 1 nbsp 10 9 4 10 2 10 10 10 10 1 displaystyle 10 uparrow uparrow uparrow uparrow uparrow 2 10 uparrow uparrow uparrow uparrow 10 10 uparrow uparrow uparrow 10 1 nbsp 10 2 5 10 10 4 2 3 2 2 2 3 8 3 2 2 2 3 2 9 3 3 8 10 10 10 10 2 11 10 2 2 2 10 2 100 10 10 2 2 10 2 10 10 displaystyle 10 10 nbsp 10 10 10 10 displaystyle 10 uparrow 10 10 10 nbsp The second term in the definition of Graham s number g2 3 g1 3 gt 10 g1 1 10 10 10 3 2 10 10 10 10 10 10 displaystyle 10 10 nbsp 10 10 10 10 10 10 displaystyle 10 uparrow 10 uparrow 10 10 10 10 nbsp g3 3 3 g2 gt 10 10 g2 1 gt 10 10 3 2 g4 3 3 g3 gt 10 10 g3 1 gt 10 10 4 2 g9 3 3 g8 is between 10 10 9 2 and 10 10 10 2 10 10 10 2 g10 3 3 g9 is between 10 10 10 2 and 10 10 11 2 g63 3 3 g62 is between 10 10 63 2 and 10 10 64 2 10 10 64 2 Graham s number g64 12 10 10 65 2 10 10 10 3 10 10 10 4 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 10 where there are 10 10 10 10 s Other notations edit Some notations for extremely large numbers Knuth s up arrow notation hyperoperators Ackermann function including tetration Conway chained arrow notation Steinhaus Moser notation apart from the method of construction of large numbers this also involves a graphical notation with polygons Alternative notations like a more conventional function notation can also be used with the same functions Fast growing hierarchy These notations are essentially functions of integer variables which increase very rapidly with those integers Ever faster increasing functions can easily be constructed recursively by applying these functions with large integers as argument A function with a vertical asymptote is not helpful in defining a very large number although the function increases very rapidly one has to define an argument very close to the asymptote i e use a very small number and constructing that is equivalent to constructing a very large number e g the reciprocal Comparison of base values editThe following illustrates the effect of a base different from 10 base 100 It also illustrates representations of numbers and the arithmetic 100 12 10 24 displaystyle 100 12 10 24 nbsp with base 10 the exponent is doubled 100 100 12 10 2 10 24 displaystyle 100 100 12 10 2 10 24 nbsp ditto 100 100 100 12 10 10 2 10 24 0 30103 displaystyle 100 100 100 12 approx 10 10 2 10 24 0 30103 nbsp the highest exponent is very little more than doubled increased by log102 100 2 10 200 displaystyle 100 uparrow uparrow 2 10 200 nbsp 100 3 10 2 10 200 displaystyle 100 uparrow uparrow 3 10 2 times 10 200 nbsp 100 4 10 2 2 10 200 0 3 10 2 2 10 200 10 3 200 3 10 4 2 3 displaystyle 100 uparrow uparrow 4 10 uparrow 2 2 times 10 200 0 3 10 uparrow 2 2 times 10 200 10 uparrow 3 200 3 10 uparrow 4 2 3 nbsp 100 n 10 n 2 2 10 200 10 n 1 200 3 10 n 2 3 lt 10 n 1 displaystyle 100 uparrow uparrow n 10 uparrow n 2 2 times 10 200 10 uparrow n 1 200 3 10 uparrow n 2 3 lt 10 uparrow uparrow n 1 nbsp thus if n is large it seems fair to say that 100 n displaystyle 100 uparrow uparrow n nbsp is approximately equal to 10 n displaystyle 10 uparrow uparrow n nbsp 100 2 10 98 2 10 200 10 100 2 3 displaystyle 100 uparrow uparrow uparrow 2 10 uparrow 98 2 times 10 200 10 uparrow 100 2 3 nbsp 100 3 10 10 98 2 10 200 10 10 100 2 3 displaystyle 100 uparrow uparrow uparrow 3 10 uparrow uparrow 10 uparrow 98 2 times 10 200 10 uparrow uparrow 10 uparrow 100 2 3 nbsp 100 n 10 n 2 10 98 2 10 200 10 n 2 10 100 2 3 lt 10 n 1 displaystyle 100 uparrow uparrow uparrow n 10 uparrow uparrow n 2 10 uparrow 98 2 times 10 200 10 uparrow uparrow n 2 10 uparrow 100 2 3 lt 10 uparrow uparrow uparrow n 1 nbsp compare 10 n 10 n 2 10 10 1 lt 10 n 1 displaystyle 10 uparrow uparrow uparrow n 10 uparrow uparrow n 2 10 uparrow 10 1 lt 10 uparrow uparrow uparrow n 1 nbsp thus if n is large it seems fair to say that 100 n displaystyle 100 uparrow uparrow uparrow n nbsp is approximately equal to 10 n displaystyle 10 uparrow uparrow uparrow n nbsp 100 2 10 98 10 100 2 3 displaystyle 100 uparrow uparrow uparrow uparrow 2 10 uparrow uparrow 98 10 uparrow 100 2 3 nbsp compare 10 2 10 8 10 10 1 displaystyle 10 uparrow uparrow uparrow uparrow 2 10 uparrow uparrow 8 10 uparrow 10 1 nbsp 100 3 10 10 98 10 100 2 3 displaystyle 100 uparrow uparrow uparrow uparrow 3 10 uparrow uparrow uparrow 10 uparrow uparrow 98 10 uparrow 100 2 3 nbsp compare 10 3 10 10 8 10 10 1 displaystyle 10 uparrow uparrow uparrow uparrow 3 10 uparrow uparrow uparrow 10 uparrow uparrow 8 10 uparrow 10 1 nbsp 100 n 10 n 2 10 98 10 100 2 3 displaystyle 100 uparrow uparrow uparrow uparrow n 10 uparrow uparrow uparrow n 2 10 uparrow uparrow 98 10 uparrow 100 2 3 nbsp compare 10 n 10 n 2 10 8 10 10 1 displaystyle 10 uparrow uparrow uparrow uparrow n 10 uparrow uparrow uparrow n 2 10 uparrow uparrow 8 10 uparrow 10 1 nbsp if n is large this is approximately equal Accuracy editFor a number 10 n displaystyle 10 n nbsp one unit change in n changes the result by a factor 10 In a number like 10 6 2 10 3 displaystyle 10 6 2 times 10 3 nbsp with the 6 2 the result of proper rounding using significant figures the true value of the exponent may be 50 less or 50 more Hence the result may be a factor 10 50 displaystyle 10 50 nbsp too large or too small This seems like extremely poor accuracy but for such a large number it may be considered fair a large error in a large number may be relatively small and therefore acceptable For very large numbers edit In the case of an approximation of an extremely large number the relative error may be large yet there may still be a sense in which one wants to consider the numbers as close in magnitude For example consider 10 10 displaystyle 10 10 nbsp and 10 9 displaystyle 10 9 nbsp The relative error is 1 10 9 10 10 1 1 10 90 displaystyle 1 frac 10 9 10 10 1 frac 1 10 90 nbsp a large relative error However one can also consider the relative error in the logarithms in this case the logarithms to base 10 are 10 and 9 so the relative error in the logarithms is only 10 The point is that exponential functions magnify relative errors greatly if a and b have a small relative error 10 a displaystyle 10 a nbsp and 10 b displaystyle 10 b nbsp the relative error is larger and 10 10 a displaystyle 10 10 a nbsp and 10 10 b displaystyle 10 10 b nbsp will have an even larger relative error The question then becomes on which level of iterated logarithms do to compare two numbers There is a sense in which one may want to consider 10 10 10 displaystyle 10 10 10 nbsp and 10 10 9 displaystyle 10 10 9 nbsp to be close in magnitude The relative error between these two numbers is large and the relative error between their logarithms is still large however the relative error in their second iterated logarithms is small log 10 log 10 10 10 10 10 displaystyle log 10 log 10 10 10 10 10 nbsp and log 10 log 10 10 10 9 9 displaystyle log 10 log 10 10 10 9 9 nbsp Such comparisons of iterated logarithms are common e g in analytic number theory Classes edit One solution to the problem of comparing large numbers is to define classes of numbers such as the system devised by Robert Munafo 13 which is based on different levels of perception of an average person Class 0 numbers between zero and six is defined to contain numbers that are easily subitized that is numbers that show up very frequently in daily life and are almost instantly comparable Class 1 numbers between six and 1 000 000 106 is defined to contain numbers whose decimal expressions are easily subitized that is numbers who are easily comparable not by cardinality but at a glance given the decimal expansion Each class after these are defined in terms of iterating this base 10 exponentiation to simulate the effect of another iteration of human indistinguishibility For example class 5 is defined to include numbers between 101010106 and 10101010106 which are numbers where X becomes humanly indistinguishable from X2 14 taking iterated logarithms of such X yields indistinguishibility firstly between log X and 2log X secondly between log log X and 1 log log X and finally an extremely long decimal expansion whose length can t be subitized Approximate arithmetic edit There are some general rules relating to the usual arithmetic operations performed on very large numbers The sum and the product of two very large numbers are both approximately equal to the larger one 10 a 10 b 10 a 10 b 10 10 b log 10 a displaystyle 10 a 10 b 10 a10 b 10 10 b log 10 a nbsp Hence A very large number raised to a very large power is approximately equal to the larger of the following two values the first value and 10 to the power the second For example for very large n displaystyle n nbsp there is n n 10 n displaystyle n n approx 10 n nbsp see e g the computation of mega and also 2 n 10 n displaystyle 2 n approx 10 n nbsp Thus 2 65536 10 65533 displaystyle 2 uparrow uparrow 65536 approx 10 uparrow uparrow 65533 nbsp see table Systematically creating ever faster increasing sequences editMain article fast growing hierarchy Given a strictly increasing integer sequence function f 0 n displaystyle f 0 n nbsp n 1 it is possible to produce a faster growing sequence f 1 n f 0 n n displaystyle f 1 n f 0 n n nbsp where the superscript n denotes the nth functional power This can be repeated any number of times by letting f k n f k 1 n n displaystyle f k n f k 1 n n nbsp each sequence growing much faster than the one before it Thus it is possible to define f w n f n n displaystyle f omega n f n n nbsp which grows much faster than any f k displaystyle f k nbsp for finite k here w is the first infinite ordinal number representing the limit of all finite numbers k This is the basis for the fast growing hierarchy of functions in which the indexing subscript is extended to ever larger ordinals For example starting with f0 n n 1 f1 n f0n n n n 2n f2 n f1n n 2nn gt 2 n for n 2 using Knuth up arrow notation f3 n f2n n gt 2 n n 2 2 n for n 2 fk 1 n gt 2 k n for n 2 k lt w fw n fn n gt 2 n 1 n gt 2 n 2 n 3 3 A n n for n 2 where A is the Ackermann function of which fw is a unary version fw 1 64 gt fw64 6 gt Graham s number g64 in the sequence defined by g0 4 gk 1 3 gk 3 This follows by noting fw n gt 2 n 1 n gt 3 n 2 3 2 and hence fw gk 2 gt gk 1 2 fw n gt 2 n 1 n 2 n n 1 2 n n 1 1 using Conway chained arrow notation fw 1 n fwn n gt 2 n n 1 2 because if gk n X n k then X n k 1 gkn 1 fw k n gt 2 n n 1 k 1 gt n n k fw2 n fw n n gt n n n n n n 1 fw2 k n gt n n n k fw3 n gt n n n n fwk n gt n n n n Chain of k 1 n s fw2 n fwn n gt n n n n Chain of n 1 n s In some noncomputable sequences editThe busy beaver function S is an example of a function which grows faster than any computable function Its value for even relatively small input is huge The values of S n for n 1 2 3 4 are 1 4 6 13 sequence A028444 in the OEIS S 5 is not known but is definitely 4098 S 6 is at least 10 15 Infinite numbers editMain article cardinal number See also large cardinal Mahlo cardinal and totally indescribable cardinal Although all the numbers discussed above are very large they are all still decidedly finite Certain fields of mathematics define infinite and transfinite numbers For example aleph null is the cardinality of the infinite set of natural numbers and aleph one is the next greatest cardinal number c displaystyle mathfrak c nbsp is the cardinality of the reals The proposition that c ℵ 1 displaystyle mathfrak c aleph 1 nbsp is known as the continuum hypothesis See also editArbitrary precision arithmetic List of arbitrary precision arithmetic software Dirac large numbers hypothesis Exponential growth History of large numbers Human scale Indefinite and fictitious numbers Largest number Infinity Law of large numbers Myriads 10 000 in East Asia Names of large numbers Power of two Power of 10 TetrationReferences edit One Million Things A Visual Encyclopedia unreliable source The study of large numbers is called googology unreliable source Bianconi Eva Piovesan Allison Facchin Federica Beraudi Alina Casadei Raffaella Frabetti Flavia Vitale Lorenza Pelleri Maria Chiara Tassani Simone Nov Dec 2013 An estimation of the number of cells in the human body Annals of Human Biology 40 6 463 471 doi 10 3109 03014460 2013 807878 hdl 11585 152451 ISSN 1464 5033 PMID 23829164 S2CID 16247166 Landenmark HK Forgan DH Cockell CS June 2015 An Estimate of the Total DNA in the Biosphere PLOS Biology 13 6 e1002168 doi 10 1371 journal pbio 1002168 PMC 4466264 PMID 26066900 Nuwer R 18 July 2015 Counting All the DNA on Earth The New York Times New York ISSN 0362 4331 Retrieved 2015 07 18 Shannon Claude March 1950 XXII Programming a Computer for Playing Chess PDF Philosophical Magazine Series 7 41 314 Archived from the original PDF on 2010 07 06 Retrieved 2019 01 25 Atoms in the Universe Universe Today 30 07 2009 Retrieved 02 03 13 Information Loss in Black Holes and or Conscious Beings Don N Page Heat Kernel Techniques and Quantum Gravity 1995 S A Fulling ed p 461 Discourses in Mathematics and its Applications No 4 Texas A amp M University Department of Mathematics arXiv hep th 9411193 ISBN 0 9630728 3 8 How to Get A Googolplex Carl Sagan takes questions more from his Wonder and Skepticism CSICOP 1994 keynote Skeptical Inquirer Archived December 21 2016 at the Wayback Machine GIMPS Discovers Largest Known Prime Number Great Internet Mersenne Prime Search 2018 12 21 Regarding the comparison with the previous value 10 n 10 lt 3 n 1 3 displaystyle 10 uparrow n 10 lt 3 uparrow n 1 3 nbsp so starting the 64 steps with 1 instead of 4 more than compensates for replacing the numbers 3 by 10 Large Numbers at MROB www mrob com Retrieved 2021 05 13 Large Numbers page 2 at MROB www mrob com Retrieved 2021 05 13 Retrieved from https en wikipedia org w index php title Large numbers amp oldid 1221450925, wikipedia, wiki, book, books, library,

article

, read, download, free, free download, mp3, video, mp4, 3gp, jpg, jpeg, gif, png, picture, music, song, movie, book, game, games.