Exponentiation with arbitrary bases, exponents - Vipul Naik files vipulnaik com/math-152/arbitraryexponents pdf (2) All the laws of exponents that we are familiar with for integer and rational to use divide-and-conquer strategies that work by breaking a problem up
Exponents and Polynomials - Palm Beach State College www palmbeachstate edu/prepmathLW/documents/BeginningAlgebra7eChapter5 pdf exponents and exponential expressions an especially useful type of exponential expression is a polynomial polynomials model many real- world phenomena
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Powers of 10 & Scientific Notation www phys hawaii edu/~nassir/phys151/handouts/scinothandout-11spr pdf Note: Scientists and engineers sometimes break rules (1) and (2) in order to make the power n a multiple of 3; i e , we favor the powers 103, 106, 109,
6 2 Properties of Logarithms www shsu edu/~kws006/Precalculus/3 3_Logarithms_files/S 26Z 206 2 20 26 206 3 pdf (Inverse Properties of Exponential and Log Functions) Let b > 0, b = 1 to a property of exponents that we have broken tradition with the vast majority
Boolean Exponent Splitting - SciTePress www scitepress org/Papers/2021/105709/105709 pdf vantage over previous examples of exponent split- ting (Clavier and Joye, 2001; location attack to successfully break the security of our algorithms
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logarithm to positive base. The method of differentiating functions where the exponent (or base of logarithm)
itself is variable. Key properties of exponents and logarithms.(2) All the laws of exponents that we are familiar with for integer and rational exponents continue to
hold. In particular,a0= 1,ab+c=ab·ac,a1=a, andabc= (ab)c.(3) The exponentiation function is continuous in the exponent variable. In particular, for a fixed value
ofa >0, the functionx?→axis continuous. Whena?= 1, it is also one-to-one with domainRandrange (0,∞), with inverse functiony?→(lny)/(lna), which is also written as loga(y). In the case
a >1, it is an increasing function, and in the casea <1, it is a decreasing function.(4) The exponentiation function is also continuous in the base variable. In particular, for a fixed value
ofb, the functionx?→xbis continuous. Whenb?= 0, it is a one-to-one function with domain andrange both (0,∞), and the inverse function isy?→y1/b. In caseb >0, the function is increasing,
and in caseb <0, the function is decreasing. (5) Actually, we can say something stronger aboutab- it isjointlycontinuous in both variables. This is hard to describe formally here, but what it approximately means is that iffandgare both continuous functions, andftakes positive values only, thenx?→[f(x)]g(x)is also continuous.(6) The derivative of the function [f(x)]g(x)is [f(x)]g(x)times the derivative of its logarithm, which is
g(x)ln(f(x)). We can further simplify this to obtain the formula: ddx ? [f(x)]g(x)? = [f(x)]g(x)?g(x)f?(x)f(x)+g?(x)ln(f(x))?(7) Special cases worth noting: the derivative of (f(x))risr(f(x))r-1f?(x) and the derivative ofag(x)
isag(x)g?(x)lna. (8) Even further special cases: the derivative ofxrisrxr-1and the derivative ofaxisaxlna. (9) The antiderivative ofxrisxr+1/(r+1)+C(forr?=-1) and ln|x|+Cforr=-1. The antiderivative ofaxisax/(lna) +Cfora?= 1 andx+Cfora= 1. (10) The logarithm log a(b) is defined as (lnb)/(lna). This is called the logarithm ofbto basea. Note that this is defined whenaandbare both positive anda?= 1. This satisfies a bunch of identities, most of which are direct consequences of identities for the natural logarithm. In particular, log a(bc) = loga(b)+loga(c), loga(b)logb(c) = loga(c), loga(1) = 0, loga(a) = 1, loga(ar) =r, loga(b)·logb(a) = 1
and so on.(1) We can use the formulas here to differentiate expressions of the formf(x)g(x), and even to differentiate
longer exponent towers (such asxxxand 22x). (2) To solve an integration problem with exponents, it may be most prudent to rewriteabas exp(blna) and work from there onward using the rules mastered earlier. Similarly, when dealing with relative logarithms, it may be most prudent to convert all expressions in terms of natural logairthms and then use the rules mastered earlier. 1(1)bis a positive integer: In this case,abis defined as the product ofawith itselfbtimes. This definition
is fairly general; in fact, it makes sense even whena <0. (2)bis an integer: Ifbis positive, we use (1). Ifb= 0, we defineabas 1, and ifb <0, we defineabasFor the rest of this document, where we study arbitrary real exponentsb, we restrict ourselves to the
situation where the baseaof exponentiation is positive.we"re doing mathematics, it might help to think about the way mathematicians would view this. A math-
ematician would begin by defining positive exponents: things likeabwhereais a positive real andbis a positive integer. Then, the mathematician would observe thatab+c=ab·acandabc= (ab)c. The math-ematician would then ask: is there a way of extending the definition to encompass more values ofbwhile
preserving these two laws of exponents? Further, is the way more or less unique or are there multiple different
extensions?It turns out that there is a way, and it is unique, and it is exactly the way I mentioned above. In other
words, if we want exponentiation to behave such thatab+c=ab·acand if we have it defined the usual way
for positive integersb, we are forced to define it the usual way for all integersb. Further, we are forced to
define it the way we have defined it for rational numbersb. The rules constrain us.exponents. Unfortunately, the laws of exponents are not enough to force us to a specific definition ofabfor
apositive real andbreal. However, the laws of exponents, along withcontinuity in bothaandbdo turnout to be enough to force a specific definition ofab. To see this, note that we already have definedabforb
rational, and the rationals aredensein the reals, so to figure out the answerabfor a real value ofb, we take
rationalsccloser and closer toband consider the limit ofac.However, we would ideally like a clearer description that does not involve this approximation procedure.
It turns out that the exponentiation function (obtained as the inverse function to the natural logarithm
function) works out.Note that I use the exp notation because I want to emphasize that exp is just the inverse function to ln;
it does not have ana priorimeaning as exponentation. Note that this definition coincides with the usual
definition for positive integer exponents, becauseab=a·a· ··· ·a btimes, and thus we get:
ln(ab) =blnafor negative integer exponents and for all rational exponents. Thus, this new definition extends the old
definition. Next, we can use the properties of exponents and logarithms to verify: (1) With this new definition, the general laws for exponents listed above continue to hold. (2) Under this new definition of exponent,abis continuous in each variable. In other words, for anyfixeda, it is a continuous function ofb, and for a fixedb, it is a continuous function ofa. Actually,
something stronger holds; it is jointly continuous in the two variables. However, joint continuity is
a concept that is based on ideas of multivariable calculus, and hence beyond our scope.(3) For a fixeda?= 1, the functionx?→axis a one-to-one function fromRto (0,∞). Whena >1 the
function is increasing, and whena <1, the function is decreasing.(4) For a fixedb?= 0, the function is a one-to-one function from (0,∞) to (0,∞). Whenb >0, it is an
increasing function, and whenb <0, it is a decreasing function.is subtraction, and theinverse operationcorresponding to multiplication is division. What is the inverse
operation corresponding to exponentiation? The answer turns out to be tricky, because there are a couple
of nice things about addition and multiplication that are no longer true for exponentiation: (1) Addition and multiplication are bothcommutative: We have the remarkable fact thata+b=b+a andab=bafor anyaandb. On the other hand, exponentiation is not commutative. In fact, as we might see some time later, for everya?(0,∞), there exist at most two values ofb?(0,∞) such thatab=ba, and one of those two values isa. For instance, the only numbersbfor which 2b=b2 areb= 2 andb= 4. (2) Addition and multiplication are bothassociative: We have the remarkable fact thata+ (b+c) = (a+b) +canda(bc) = (ab)c. On the other hand, exponentiation is notassociative, i.e., it is not true in general thata(bc)= (ab)c. This is because (ab)c=abc, and so the equality would give that b c=bc, which is very rare. The noncommutativity of exponentiation would mean that there are two notions of inverse operation: aleft inverse operation and a right inverse operation. The nonassociativity would mean that these inverse
operations behave very differently from subtraction and division, and the analogy cannot be stretched too
far.Note that as per our general discussion of theabfunction, we see that this is well-defined and unique if
b?= 0. The other kind of inverse operation we may want is to solve the equation: a x=cNote that the uniqueness ofxcorresponds to the fact, observed earlier, that for fixeda, the mapx?→ax
is one-to-one.This is often read aslogarithm ofcto basea. The mapc?→loga(c) is calledtaking logarithms to basea.
As shown above, it is equivalent to taking natural logarithms and dividing by lna.that all elements appearing in the base of the logarithm are positive and not equal to 1, and all elements
whose logarithm is being taken are positive: log a(bc) = loga(b) + loga(c) log a(bc) =cloga(b) log a(1/b) =-loga(b) log a(1) = 0 log a(a) = 1 log a(ar) =r logAll of these follow from the definition and the corresponding properties of ln, which follow from its
definition as the antiderivative of the reciprocal function. 4logarithm to a given base as measuring arelative logarithm. The natural logarithm is the logarithm to
basee, which is thenatural logarithm, in that the baseeis the natural choice for a base. This behavior of
logarithms is very similar to, for instance, the behavior of refractive indices for pairs of media through which
light travels. For any pair of media, we can define a refractive index of the pair, but thenatural basewith
respect to which we measure refractive index is vacuum. Natural logarithms play the role of vacuum: the
natural base choice. There are two other common choices of base for logarithms. One is base 10, which has no sound mathe-matical reason. The reason for taking logarithms to base 10 is because it is easy to compute the logarithm
of any number by writing it in scientific notation using a table of logarithm values for numbers from 1 to
The second natural choice of base for logarithms, which we will talk about next time, is logarithms to
base 2. These come up for three reasons, listed below. We will return to some of these reasons in more detail
when we study exponential growth and decay next quarter. (1) Halving and doubling are operations to which humans relate easily. We measure and record the half-lifeof radioactive substances, talk of the time it takes for a country todoubleits GDP, and routinely hear campaign rhetoric and promotional NGO material that talks ofdoublingandhalvingarbitrary indicators. The reason is not that 2 has any special mathematical or real-world significance
(or plausibility, in the case of politicians and NGOs) but rather, that it is easy for people to (believe
they) understand. It"s a lot less exciting to make a campaign promise to multiply the number of tax breaks or subsidies or scholarships bye, even thoughe >2. (2) The second reason is perhaps more legitimate. In computer science algorithms, it is customary to usedivide-and-conquer strategiesthat work by breaking a problem up into two roughly equal subproblems, and solving both of them separately. The amount of time and resources needed to solve problems using such strategies typically involves a logarithm to base 2, since that is the number of times you need to keep dividing the problem into two equal parts until you get to problems of size(3) The third reason has to do with biology, more specifically with the reproduction strategies of some
unicellular organisms. These organisms divide into two organisms. This form of asexual reproduction is termedbinary fission. Other reproduction strategies or behaviors may also be associated with logarithms to base 2 or 3, because of the discrete nature of numbers of offspring and number of parents.One way of thinking about this is that logarithms to base 2 are more natural when working withfinite,
discrete problemswhile logarithms to baseeare more common when dealing withcontinuous processes.the general procedure for differentiation the functionf(x)g(x), wherefis a positive-valued function andgis
a real-valued function.(2) The case wheref(x) is a constant function with valuea. In this case, the derivative isag(x)g?(x)lna.
In the further special case whereg(x) =x, we obtainaxlna. In other words, the derivative ofax with respect toxisaxlna.Note: We don"t need to put the|x|in the ln antiderivative if the exponent is irrational becausexrisn"t
even defined for irrational exponents, so lnx+Cis a valid answer for irrational exponents.When you double the lengths, the areas become four times their original value, and the volumes become
eight times their original value. More generally, when you scale lengths by a factor ofλ, the areas get scaled
by a factor ofλ2, and the volumes gets scaled by a factor ofλ3. Theexponentof 2 occurs because area is two-dimensional and the exponent of 3 occurs because volume is three-dimensional.Suppose there is a certain physical quantity such that, when we scale lengths by a factor ofλ?= 1, that
quantity scales by a factor ofμ. What is the dimension of that quantity? It is the valuedsuch thatλd=μ.
With our new understanding of logarithms, we can write: d:= logλ(μ) =lnμlnλWhen we put it this bleakly, it does not seem a foregone conclusion thatdmust be a positive integer. In
fact, there is a whole range of physical objects that have positive measure infractal dimension, i.e., there
are quantities that we associate with them whose dimension is not an integer. For instance, there are certain
6sets such as Cantor sets that we design in such a way that when we triple the lengths, the size of those
objectsdoubles. Thus, the dimension of such an object is: ln2ln3 ≈0.71.1≈0.63Similarly, there are sets with the property that when you double lengths they increase by a factor of three
times. The dimension of such sets is: ln3ln2 ≈1.10.7≈1.57 7