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The uniform second-order Taylor remainder of z↦(1−z)−1/2 on [0,z0]

Statement

Let z0∈[0,1) and define f:(−∞,1)→R by f(z):=(1−z)−1/2=((1−z)1/2)−1, the reciprocal of the nonnegative square root, with rational powers as in Rational powers ar of a positive base; put K(z0):=38(1−z0)−5/2.

(a) f is differentiable on (−∞,1) with f′(z)=12(1−z)−3/2, and twice differentiable there with f′′(z)=34(1−z)−5/2; in particular ∣f′′(z)∣≤34(1−z0)−5/2 for every z∈[0,z0].

(b) For every z∈[0,z0] there is a real R(z) with f(z)=1+z2+R(z),∣R(z)∣≤K(z0) z2, so ∣f(z)−1∣≤z2+K(z0)z2 for z∈[0,z0]. Consequently, for every η>0, 0≤z≤min⁡ ⁣{z0,η12+K(z0)z0} ⟹ ∣f(z)−1∣≤η; the display is the quantitative form of f(z)→1 as z→0+ used by Uniform Galilean limit of the boost charts on bounded regions, and its failure on the whole chart domain.

The lemma is a statement of real analysis about the single function f; it attaches no physical meaning to z and makes no claim about a Lorentz factor or a physical velocity.

Facts & Assumptions

Given: A real number z0∈[0,1); the function f:(−∞,1)→R, f(z)=(1−z)−1/2=((1−z)1/2)−1, with rational powers as in Rational powers ar of a positive base; and the constant K(z0)=38(1−z0)−5/2.

[L1]

For a>0 and rational r the rational power ar is defined and positive, and a−r=(ar)−1; on rational exponents it agrees with the real power exp⁡(rlog⁡a) (Rational powers ar of a positive base, Laws of rational exponents, The exponential definition of real powers agrees with the existing rational powers). In particular 1−1/2=1.

[L2]

For real α the function x↦xα is differentiable on (0,∞) with derivative αxα−1 (Continuity and derivatives of positive-base real powers).

[L4]

If 0≤z≤z0 then 0<1−z0≤1−z, and for positive bases a≤b and rational r>0 one has ar≤br (with equality exactly when a=b); reciprocals of positive elements reverse the order (Monotonicity of r↦ar and of a↦ar, Inverses of positives are positive, and reciprocation reverses order).

[L5]

Taylor's theorem with the Lagrange remainder: if f has derivatives through order n+1 on the closed interval between a and x with endpoint continuity, and ∣f(n+1)(t)∣≤M throughout that interval, then ∣Rn,af(x)∣≤M ∣x−a∣n+1/(n+1)! (A uniform derivative bound gives a uniform Taylor remainder bound).

[L6]

Absolute value: ∣u+v∣≤∣u∣+∣v∣, ∣uv∣=∣u∣ ∣v∣, ∣u∣=u for u≥0, and ∣u∣=0 if and only if u=0 (Absolute value in an ordered field, Basic properties of the absolute value, The triangle inequality).

[L7]

The canonical natural numbers are cofinal in R: for every real b there is an integer N>b (Every complete ordered field is Archimedean).

Proof

technique · direct
1.1givenL1L2

The composite form of f. Define g:(−∞,1)→(0,∞) by g(z):=1−z and h:(0,∞)→(0,∞) by h(y):=y−1/2. For every z<1 the base 1−z is positive, so f=h∘g; and by [L1] the rational power h(y)=y−1/2 equals the real power exp⁡(−12log⁡y), so the derivative statement of [L2] applies to h.

1.2L3

The inner derivative. The constant function z↦1 has derivative 0 and the identity p1 has p1′≡1 by [L3]; the difference rule of Sums, scalar multiples, products and quotients: (f+g)′(c)=f′(c)+g′(c), (αf)′(c)=αf′(c), (fg)′(c)=f′(c)g(c)+f(c)g′(c), and (f/g)′(c)=(f′(c)g(c)−f(c)g′(c))/g(c)2 when g(c)≠0 therefore gives g′(z)=−1 for every z∈(−∞,1), and each point of (−∞,1) is a limit point of that interval.

2.1L2step 1.1

The outer derivative. By [L2] with α=−12, the function y↦y−1/2 is differentiable on (0,∞) with derivative (y−1/2)′=−12y−3/2; by step 1.1 this is h′.

3.1step 1.2step 2.1L3algebra

First derivative of f. Fix z∈(−∞,1). Then g(z)=1−z>0 is a limit point of (0,∞), so the chain rule [L3] applied to f=h∘g at z gives f′(z)=h′(g(z))g′(z)=−12(1−z)−3/2⋅(−1)=12(1−z)−3/2.

4.1step 3.1L1L2L3algebra

Second derivative of f. The function z↦12(1−z)−3/2 is the scalar multiple by 12 of the composite of g with y↦y−3/2; the rational power y−3/2 agrees with the real power by [L1], so [L2] with α=−32 gives it derivative −32y−5/2 on (0,∞), and the scalar rule and the chain rule [L3] give f′′(z)=12(−32(1−z)−5/2)(−1)=34(1−z)−5/2 for every z∈(−∞,1), which also covers the claim that f is twice differentiable there.

5.1step 4.1L1L4L6algebra

Uniform bound on [0,z0]. Let z∈[0,z0]. By [L4], 0<1−z0≤1−z, so (1−z0)5/2≤(1−z)5/2 and, taking reciprocals of positive elements, (1−z)−5/2≤(1−z0)−5/2. Multiplying by 34>0 and using f′′>0 by [L1] to read ∣f′′∣=f′′ ([L6]) gives ∣f′′(z)∣=f′′(z)≤34(1−z0)−5/2 for every z∈[0,z0].

6.1step 3.1step 5.1L1L5algebra

The Taylor remainder. Fix z∈[0,z0]. Since [0,z]⊆(−∞,1), the function f has derivatives through order 2 on the closed interval between 0 and z, continuous at the endpoints; by step 5.1 the second derivative is bounded there by M:=34(1−z0)−5/2. Applying [L5] with n=1, a=0 and this z gives, for R(z):=R1,0f(z)=f(z)−f(0)−f′(0)z, ∣R(z)∣≤M2! z2=38(1−z0)−5/2z2=K(z0)z2. Here f(0)=1−1/2=1 by [L1] and f′(0)=12 by step 3.1, so the displayed expansion of f is f(z)=1+z2+R(z).

7.1step 6.1L1L6algebra

The quantitative limit. For z∈[0,z0], steps 6.1 and 3.1 give ∣f(z)−1∣=∣z2+R(z)∣≤z2+K(z0)z2=z(12+K(z0)z)≤z(12+K(z0)z0) by [L6] and K(z0)>0, z≤z0, which is the first displayed assertion of (b); if in addition 0≤z≤η/(12+K(z0)z0) for an η>0, then ∣f(z)−1∣≤η, which is the second displayed assertion; and the bound is not asserted for z outside [0,z0].

8.1step 6.1L1L6L7algebra∎

Failure of a single remainder constant on [0,1). For every integer N≥2 put zN=1−N−2∈(0,1). By [L1], f(zN)=N, so the exact remainder rN:=f(zN)−1−zN/2=N−1−zN/2 satisfies rN>N−3/2. Given B≥0, choose N>max⁡{2,B+3/2} by [L7]; then ∣rN∣>B≥BzN2. Thus no finite B≥0 bounds ∣f(z)−1−z/2∣ by Bz2 on all of [0,1).

Remarks

The constants depend on z0 alone, and the estimate is uniform over the whole interval [0,z0]; as z0↑1 the constant K(z0)=38(1−z0)−5/2 grows without bound. The actual impossibility of a single remainder constant on [0,1) is proved by the family in step 8.1, which explains the bounded speed window in the consumers. No physical quantity and no physical restriction are introduced here: z is an arbitrary real parameter, and the two in-run consumers named in the statement are the items that apply this estimate to the model's velocities.

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