S01 · implies
Before
b>2
After
\int_2^b3x^{-2}\,dx=[-3/x]_2^b=3/2-3/bConditions: b>2
Rule: FTC · Uses: G1
Leaf basis: FTC
First integrate on a qualified finite interval, without directly substituting an infinite endpoint.
derivation-mko-improper-integral-01 · ocme-new142-reader-adoption-20261021
Compute three explicit power-law improper integrals and distinguish principal value.
Only complete piecewise power laws, not general integrability from finite cutoffs.
algebraepsilonFTCdefinition_herelog_integral_boundaryG1 — One side: f(x)=3/x^2 for x≥2. Two sides: g(x)=2/|x|^2 for x≤-1, zero for -1<x<1, and 3/x^2 for x≥1.G2 — Singularity example: h(x)=(-x)^(-1/2) for -1≤x<0 and 2*x^(-1/2) for 0<x≤1, split at zero.A,B,b — independent infinite-end cutoffs\delta — one-sided singular cutoff\operatorname{PV} — symmetric principal valuemko_definition · cited — A one-sided integral int_a^infinity f, from a to infinity, is the limit of finite-cutoff integrals as b→infinity; this slice declares f(x)=scale/x^p on [lower,infinity). The two-sided exact family declares f(x)=left_scale/|x|^p on x≤−1, f(x)=0 on −1<x<1 and f(x)=right_scale/x^p on x≥1; its tails must converge separately. An interior-singularity family explicitly gives both power-law pieces on [c−1,c+1] and splits at c. A symmetric principal value is insufficient. Absolute convergence is sufficient but not necessary, and apparently stable finite cutoffs do not prove convergence. · mko-improper-integralalgebra · prerequisite — Use real-field identities; division requires a nonzero denominator and multiplication by a positive number preserves inequalities.epsilon · prerequisite — Convergence requires for every positive epsilon an integer N controlling every n≥N by a strict error bound; use the Archimedean property of the reals.FTC · prerequisite — For continuous power laws on finite closed intervals use the fundamental theorem of calculus; the derivative of -c/x is c/x^2, and that of 2sqrt(x) is x^(-1/2) for x>0.definition_here · prerequisite — An ordinary improper integral requires a finite limit of finite-cutoff integrals separately at each infinite endpoint and each side of an interior singularity, then adds them; principal value separately binds symmetric cutoffs.log_integral_boundary · prerequisite — For nonzero reals the derivative of log|x| is 1/x, and log B tends to infinity as B tends to infinity.Before
b>2
After
\int_2^b3x^{-2}\,dx=[-3/x]_2^b=3/2-3/bConditions: b>2
Rule: FTC · Uses: G1
Leaf basis: FTC
First integrate on a qualified finite interval, without directly substituting an infinite endpoint.
Before
3/b\to0\quad(b\to\infty)
After
\int_2^\infty3x^{-2}\,dx=3/2Conditions: none
Rule: definition_here · Uses: S01
Leaf basis: definition_here
For any epsilon, b>3/epsilon controls the entire tail strictly, defining the one-sided integral.
Before
A>1,\ B>1
After
\int_{-A}^{-1}g=2-2/A,\quad\int_1^B g=3-3/BConditions: none
Rule: FTC · Uses: G1
Leaf basis: FTC
Use u=-x on the left and integrate directly on the right; the two cutoffs are independent.
Before
A\to\infty\text{ independently of }B\to\inftyAfter
\int_{-\infty}^{\infty}g=2+0+3=5Conditions: none
Rule: definition_here · Uses: S03
Leaf basis: definition_here
Both tails exist separately, and only then are they added to the zero middle part.
Before
0<\delta<1
After
\int_{-1}^{-\delta}h=2-2\sqrt\delta,\quad\int_{\delta}^{1}h=4-4\sqrt\deltaConditions: 0<\delta<1
Rule: FTC · Uses: G2
Leaf basis: FTC
Each side of the singularity has its own finite integral; substitute u=-x on the left and retain scale 2 on the right.
Before
\sqrt\delta\to0\quad(\delta\downarrow0)
After
\int_{-1}^{1}h=2+4=6Conditions: none
Rule: definition_here · Uses: S05
Leaf basis: definition_here
The condition delta<epsilon^2 makes sqrt(delta)<epsilon; add the two finite one-sided limits.
Before
j(x)=1/x\quad(|x|\ge1),\qquad j(x)=0\quad(|x|<1)
After
\int_{-A}^{-1}j=-\log A,\quad\int_1^B j=\log BConditions: (\log|x|)'=1/x,\quad\log B\to\infty
Rule: log_integral_boundary · Uses: G1, log_integral_boundary
Leaf basis: log_integral_boundary
In this contrast example the two tails diverge; the derivative of log|x| is 1/x, supplying its finite antiderivative.
Before
A=B\Longrightarrow-\log A+\log A=0
After
\operatorname{PV}\int j=0\text{ but the ordinary improper integral does not exist}Conditions: none
Rule: algebra · Uses: S07
Leaf basis: algebra
A zero symmetric principal value does not repair divergent individual tails and is not an ordinary improper integral.
No substeps in this guide.
S08 · premise_audit · S07 — The ordinary integral is rejected without denying the symmetric limit is zero.S07 · premise_audit · G1, log_integral_boundary — Only the stated logarithmic-antiderivative premise for this counterexample is used, not a new exp/log theory.S06 · premise_audit · S05 — A missing value at zero is not the obstruction; the one-sided integrability limits are the obligations.S05 · premise_audit · G2 — Using one symbol delta is convenient notation; the two one-sided limits must still exist separately.S04 · premise_audit · S03 — There is no symmetric cancellation; each side is independently qualified.S03 · premise_audit · G1 — Qualification must not rely on tying A and B together.S02 · premise_audit · S01 — This is not a conclusion from several close cutoff values.S01 · premise_audit · G1 — b>2 keeps the integrand continuous and denominators positive.Record each infinite endpoint and singularity side separately.
Symmetric cutoffs certify principal value, not independent tails.
reject — Neither one-sided limit of j is finite.reject — An ordinary improper integral requires both one-sided limits at each singularity.reject — No bound for every later cutoff is supplied.The three qualified improper integrals are 3/2, 5 and 6; contrast j has only symmetric principal value zero.
1 declared checks for this guide; only the listed expressions are covered.
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