TheoremBase

The power maps are differentiated by the chain rule; the bound follows by writing E(t) as the integral of E' between s and t, bounding the integrand by the given power bound and integrating it exactly with the power maps.

Proof

Computations with real numbers use The Real Numbers as a Type.

Proof of (i). Let N∈N0N\in\mathbb{N}_{0}. For every r∈[a,b]r\in[a,b], (rβˆ’s)N/N!(r-s)^{N}/N! is a real number, as N!β‰ 0N!\neq0 by Natural Numbers and Factorials Read in the Reals: the Order Carries Over, One Is Least, and Factorials Are Positive, Recursive and Nondecreasing (iii); so the map [a,b]β†’R[a,b]\to\mathbb{R}, r↦(rβˆ’s)N/N!r\mapsto(r-s)^{N}/N!, exists (a map given by an expression, Values, Restriction and Equality of a Map, and the Map u↦t(u)u\mapsto t(u) as a Defined Set Symbol (v)), and it is the only map [a,b]β†’R[a,b]\to\mathbb{R} with these values by Values, Restriction and Equality of a Map, and the Map u↦t(u)u\mapsto t(u) as a Defined Set Symbol (iv). By Powers with Exponents in the Natural Numbers with Zero (ii), (rβˆ’s)0=1(r-s)^{0}=1, and 0!=10!=1 by The Factorial as a Map on the Natural Numbers with Zero (ii); so ψ0(r)=1/0!=1\psi_{0}(r)=1/0!=1 for every r∈[a,b]r\in[a,b], ψ0\psi_{0} is the constant map with value 11, and it is differentiable at every point by Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (i). For N∈NN\in\mathbb{N}, 1≀N1\le N by Natural Numbers Are the Successors in Omega: One Is Least and Not a Successor of a Natural Number, the Successor Is Injective, and N Is Closed under Addition and Multiplication (ii), so 0N=00^{N}=0 by Powers in a Commutative Ring, a Field and an Ordered Field: Exponent Laws, Factorisation, Geometric Sums, Monotonicity and Bernoulli's Inequality (ii) and ψN(s)=0\psi_{N}(s)=0.

Let N∈N0N\in\mathbb{N}_{0}. By Basic Facts about Intervals of the Real Line (i), R\mathbb{R} is an interval containing two distinct points, and by Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (iii), with R\mathbb{R} in place of II, the map P:Rβ†’RP:\mathbb{R}\to\mathbb{R}, x↦xN+1x\mapsto x^{N+1}, is differentiable at every x∈Rx\in\mathbb{R} with derivative (N+1)xN(N+1)x^{N}. The map Ο„:[a,b]β†’R\tau:[a,b]\to\mathbb{R}, r↦rβˆ’sr\mapsto r-s, the sum of the identity map of [a,b][a,b], read as a map into R\mathbb{R}, and the constant map with value βˆ’s-s, is differentiable at every r∈[a,b]r\in[a,b] with derivative 1+0=11+0=1, by Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (ii), Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (i) and Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (iv). By Chain Rule for Real Functions on Intervals (i), with [a,b][a,b] and R\mathbb{R} in place of II and JJ, Ο„\tau in place of ff and PP in place of gg, the map Pβˆ˜Ο„:r↦(rβˆ’s)N+1P\circ\tau:r\mapsto(r-s)^{N+1} is differentiable at every r∈[a,b]r\in[a,b] with derivative (N+1)(rβˆ’s)N(N+1)(r-s)^{N}. By Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (v), ψN+1=1(N+1)!(Pβˆ˜Ο„)\psi_{N+1}=\frac{1}{(N+1)!}(P\circ\tau) is differentiable at every r∈[a,b]r\in[a,b] with derivative

ψN+1β€²(r)=(N+1)(rβˆ’s)N(N+1)!=(rβˆ’s)NN!=ψN(r),\psi_{N+1}'(r)=\frac{(N+1)(r-s)^{N}}{(N+1)!}=\frac{(r-s)^{N}}{N!}=\psi_{N}(r),

since (N+1)!=(N+1)β‹…N!(N+1)!=(N+1)\cdot N! and N!β‰ 0N!\neq0 by Natural Numbers and Factorials Read in the Reals: the Order Carries Over, One Is Least, and Factorials Are Positive, Recursive and Nondecreasing (iii), and N+1β‰ 0N+1\neq0 in R\mathbb{R}: N+1∈NN+1\in\mathbb{N} by Natural Numbers Are the Successors in Omega: One Is Least and Not a Successor of a Natural Number, the Successor Is Injective, and N Is Closed under Addition and Multiplication (i) and Natural Numbers Are the Successors in Omega: One Is Least and Not a Successor of a Natural Number, the Successor Is Injective, and N Is Closed under Addition and Multiplication (v), so 1≀N+11\le N+1 in R\mathbb{R} by Natural Numbers and Factorials Read in the Reals: the Order Carries Over, One Is Least, and Factorials Are Positive, Recursive and Nondecreasing (ii).

Every N∈N0N\in\mathbb{N}_{0} is 00 or m+1m+1 for some m∈N0m\in\mathbb{N}_{0}, by Omega Is the Least Inductive Class: It Is a Set, Induction from Zero, the Peano Properties, and Transitivity (vii) and Natural Numbers Are the Successors in Omega: One Is Least and Not a Successor of a Natural Number, the Successor Is Injective, and N Is Closed under Addition and Multiplication (v). So every ψN\psi_{N}, N∈N0N\in\mathbb{N}_{0}, is differentiable at every point of [a,b][a,b], hence differentiable on [a,b][a,b], and continuous at every point of [a,b][a,b] by The Increment Form of the Derivative, and Differentiability Implies Continuity (ii), hence continuous on [a,b][a,b] (Continuous Map Between Metric Spaces (ii)). This proves (i).

Proof of (ii). Let p,q,c,Np,q,c,N and EE be as there, and let t∈[a,b]t\in[a,b]. As N+1∈NN+1\in\mathbb{N} (Natural Numbers Are the Successors in Omega: One Is Least and Not a Successor of a Natural Number, the Successor Is Injective, and N Is Closed under Addition and Multiplication (i) and Natural Numbers Are the Successors in Omega: One Is Least and Not a Successor of a Natural Number, the Successor Is Injective, and N Is Closed under Addition and Multiplication (v)), ψN+1(s)=0\psi_{N+1}(s)=0 by (i). Let R=cβ€‰βˆ£tβˆ’s∣N+1/(N+1)!R=c\,|t-s|^{N+1}/(N+1)!; then Rβ‰₯0R\ge0 by cβ‰₯0c\ge0, Powers in a Commutative Ring, a Field and an Ordered Field: Exponent Laws, Factorisation, Geometric Sums, Monotonicity and Bernoulli's Inequality (vi) and Natural Numbers and Factorials Read in the Reals: the Order Carries Over, One Is Least, and Factorials Are Positive, Recursive and Nondecreasing (iii). If t=st=s, then βˆ₯E(t)βˆ₯=βˆ₯0pΓ—qβˆ₯=0≀R\lVert E(t)\rVert=\lVert0_{p\times q}\rVert=0\le R by Rules for the Operator Norm: Bound, Least Constant, Definiteness, Homogeneity, Triangle Inequality and Products (iv).

Let tβ‰ st\neq s, let uu and vv be the smaller and the larger of ss and tt, so that u<vu<v, u,v∈[a,b]u,v\in[a,b] and s∈{u,v}s\in\{u,v\}, and let Ο±=1\varrho=1 if s=us=u and Ο±=βˆ’1\varrho=-1 if s=vs=v. Then ∣rβˆ’s∣=Ο±(rβˆ’s)|r-s|=\varrho(r-s) for every r∈[u,v]r\in[u,v], so ∣rβˆ’s∣N=Ο±N(rβˆ’s)N|r-s|^{N}=\varrho^{N}(r-s)^{N} by Powers in a Commutative Ring, a Field and an Ordered Field: Exponent Laws, Factorisation, Geometric Sums, Monotonicity and Bernoulli's Inequality (ii), and ∣rβˆ’s∣N/N!=Ο±NψN(r)|r-s|^{N}/N!=\varrho^{N}\psi_{N}(r).

By The Fundamental Theorem of Calculus and the Mean Value Inequality for Vector- and Matrix-Valued Maps (iii), with [a,b][a,b] in place of II and EE in place of AA, ∫uvEβ€²\int_{u}^{v}E' is defined and equals E(v)βˆ’E(u)E(v)-E(u). As E(s)=0pΓ—qE(s)=0_{p\times q}, this is E(t)βˆ’0pΓ—q=E(t)E(t)-0_{p\times q}=E(t) if t=vt=v and 0pΓ—qβˆ’E(t)=βˆ’E(t)=(βˆ’1)E(t)0_{p\times q}-E(t)=-E(t)=(-1)E(t) if t=ut=u (Additive Laws for Vectors in Rq\mathbb{R}^q and for Real pΓ—qp\times q Matrices: Group Laws and Rules for Differences (ii)); in either case βˆ₯E(t)βˆ₯=βˆ₯∫uvEβ€²βˆ₯\lVert E(t)\rVert=\bigl\lVert\int_{u}^{v}E'\bigr\rVert by Rules for the Operator Norm: Bound, Least Constant, Definiteness, Homogeneity, Triangle Inequality and Products (v). By Rules for the Riemann Integral of Vector- and Matrix-Valued Maps (viii), with [a,b][a,b] in place of II and Eβ€²E' in place of AA, ∫uvβˆ₯Eβ€²(r)βˆ₯ dr\int_{u}^{v}\lVert E'(r)\rVert\,dr is defined and

βˆ₯∫uvEβ€²βˆ₯β‰€βˆ«uvβˆ₯Eβ€²(r)βˆ₯ dr.\Bigl\lVert\int_{u}^{v}E'\Bigr\rVert\le\int_{u}^{v}\lVert E'(r)\rVert\,dr .

The map r↦βˆ₯Eβ€²(r)βˆ₯r\mapsto\lVert E'(r)\rVert is continuous on [a,b][a,b] by Continuity of Vector- and Matrix-Valued Maps: the Componentwise Criterion, Norms and Algebraic Operations (iii) and Continuity of Vector- and Matrix-Valued Maps: the Componentwise Criterion, Norms and Algebraic Operations (v), with [a,b][a,b] in place of SS. Let g=(c ϱN)ψN:[a,b]β†’Rg=(c\,\varrho^{N})\psi_{N}:[a,b]\to\mathbb{R}, the scalar multiple; it is continuous on [a,b][a,b] by (i) and Continuity of Sums and Products of Real-Valued Functions on a Metric Space (v). For r∈[u,v]r\in[u,v], by the hypothesis on Eβ€²E',

βˆ₯Eβ€²(r)βˆ₯≀cβ€‰βˆ£rβˆ’s∣NN!=c ϱNψN(r)=g(r).\lVert E'(r)\rVert\le c\,\frac{|r-s|^{N}}{N!}=c\,\varrho^{N}\psi_{N}(r)=g(r).

The maps r↦βˆ₯Eβ€²(r)βˆ₯r\mapsto\lVert E'(r)\rVert and gg are continuous on [a,b][a,b], so they are integrable on [u,v][u,v] by A Continuous Function on a Closed Interval is Riemann Integrable (ii); that is, by The Riemann Integral on a Closed Interval via Lower and Upper Integrals (vi), their restrictions to [u,v][u,v] are bounded and integrable on [u,v][u,v], with integrals ∫uvβˆ₯Eβ€²(r)βˆ₯ dr\int_{u}^{v}\lVert E'(r)\rVert\,dr and ∫uvg\int_{u}^{v}g. By Rules for the Riemann Integral: Sums, Scalar Multiples, Monotonicity, Bounds and Constants (iii), with uu and vv in place of aa and bb and these restrictions in place of ff and gg, ∫uvβˆ₯Eβ€²(r)βˆ₯ drβ‰€βˆ«uvg\int_{u}^{v}\lVert E'(r)\rVert\,dr\le\int_{u}^{v}g. By Rules for Oriented Riemann Integrals of Real-Valued Maps: Sums, Scalar Multiples, Constants, Continuous Maps, Additivity and Evaluation by an Antiderivative (iv), ∫uvψN\int_{u}^{v}\psi_{N} is defined, and by Rules for Oriented Riemann Integrals of Real-Valued Maps: Sums, Scalar Multiples, Constants, Continuous Maps, Additivity and Evaluation by an Antiderivative (ii) and Rules for Oriented Riemann Integrals of Real-Valued Maps: Sums, Scalar Multiples, Constants, Continuous Maps, Additivity and Evaluation by an Antiderivative (vi), with [a,b][a,b] in place of II and ψN+1\psi_{N+1} in place of ff, whose derivative is ψN\psi_{N} by (i),

∫uvg=c ϱN∫uvψN=c ϱN(ψN+1(v)βˆ’ΟˆN+1(u)).\int_{u}^{v}g=c\,\varrho^{N}\int_{u}^{v}\psi_{N}=c\,\varrho^{N}\bigl(\psi_{N+1}(v)-\psi_{N+1}(u)\bigr).

If s=us=u, then Ο±=1\varrho=1, Ο±N=1\varrho^{N}=1 by Powers in a Commutative Ring, a Field and an Ordered Field: Exponent Laws, Factorisation, Geometric Sums, Monotonicity and Bernoulli's Inequality (ii), t=vt=v and ψN+1(u)=0\psi_{N+1}(u)=0, so the right side is c (tβˆ’s)N+1/(N+1)!=Rc\,(t-s)^{N+1}/(N+1)!=R, as tβˆ’s=∣tβˆ’s∣t-s=|t-s|. If s=vs=v, then Ο±=βˆ’1\varrho=-1, t=ut=u and ψN+1(v)=0\psi_{N+1}(v)=0; by Powers in a Commutative Ring, a Field and an Ordered Field: Exponent Laws, Factorisation, Geometric Sums, Monotonicity and Bernoulli's Inequality (i) and Powers in a Commutative Ring, a Field and an Ordered Field: Exponent Laws, Factorisation, Geometric Sums, Monotonicity and Bernoulli's Inequality (ii), βˆ’(βˆ’1)N=(βˆ’1)N(βˆ’1)1=(βˆ’1)N+1-(-1)^{N}=(-1)^{N}(-1)^{1}=(-1)^{N+1} and (βˆ’1)N+1(tβˆ’s)N+1=(sβˆ’t)N+1(-1)^{N+1}(t-s)^{N+1}=(s-t)^{N+1}, so the right side is c (sβˆ’t)N+1/(N+1)!=Rc\,(s-t)^{N+1}/(N+1)!=R, as sβˆ’t=∣tβˆ’s∣s-t=|t-s|. Combining the inequalities, βˆ₯E(t)βˆ₯≀R\lVert E(t)\rVert\le R. As t∈[a,b]t\in[a,b] was arbitrary, this proves (ii).

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