TheoremBase

Rules for the Riemann Integral of Vector- and Matrix-Valued Maps

Continuous vector- and matrix-valued maps on an interval are integrable, and their integrals are additive, linear, compatible with constant factors and transposes, take the value (v-u)c on a constant c, and are bounded in norm by the integral of the norm.

Statement

In the settings of Single-Variable Calculus on an Interval and Euclidean Space and Real Matrices: Standing Notation, let II be an interval containing two distinct points, as in Single-Variable Calculus on an Interval (ii), let p,q,m,n∈Np,q,m,n\in\mathbb{N}, and let x,y:I→Rqx,y:I\to\mathbb{R}^{q} and A,B:I→Mp×q(R)A,B:I\to\mathcal{M}_{p\times q}(\mathbb{R}). Integrability on [u,v][u,v], the integral ∫uv\int_{u}^{v} and its being defined are as in Riemann Integral of a Vector-Valued or Matrix-Valued Map (i), Riemann Integral of a Vector-Valued or Matrix-Valued Map (ii), Riemann Integral of a Vector-Valued or Matrix-Valued Map (iii) and Riemann Integral of a Vector-Valued or Matrix-Valued Map (iv), and as in The Riemann Integral on a Closed Interval via Lower and Upper Integrals (viii) for maps I→RI\to\mathbb{R}; continuity on II refers to dRd_{\mathbb{R}} on II, dEd_{E} on Rq\mathbb{R}^{q} and dp×qd_{p\times q} on Mp×q(R)\mathcal{M}_{p\times q}(\mathbb{R}).

If xx is continuous on II, then xx is integrable on [u,v][u,v] for all u,v∈Iu,v\in I with u<vu<v, and ∫uvx\int_{u}^{v}x is defined for all u,v∈Iu,v\in I. The same holds for AA in place of xx.

Let u,v∈Iu,v\in I. If ∫uvx\int_{u}^{v}x and ∫uvy\int_{u}^{v}y are defined, then ∫uv(x(t)+y(t))dt\int_{u}^{v}\bigl(x(t)+y(t)\bigr)dt is defined and equals ∫uvx+∫uvy\int_{u}^{v}x+\int_{u}^{v}y. If ∫uvA\int_{u}^{v}A and ∫uvB\int_{u}^{v}B are defined, then ∫uv(A(t)+B(t))dt\int_{u}^{v}\bigl(A(t)+B(t)\bigr)dt is defined and equals ∫uvA+∫uvB\int_{u}^{v}A+\int_{u}^{v}B.

Let u,v∈Iu,v\in I and c∈Rc\in\mathbb{R}. If ∫uvx\int_{u}^{v}x is defined, then ∫uvc x(t) dt\int_{u}^{v}c\,x(t)\,dt is defined and equals c∫uvxc\int_{u}^{v}x. If ∫uvA\int_{u}^{v}A is defined, then ∫uvc A(t) dt\int_{u}^{v}c\,A(t)\,dt is defined and equals c∫uvAc\int_{u}^{v}A.

If xx is continuous on II, then ∫uwx=∫uvx+∫vwx\int_{u}^{w}x=\int_{u}^{v}x+\int_{v}^{w}x for all u,v,w∈Iu,v,w\in I. The same holds for AA in place of xx.

Let b∈Rqb\in\mathbb{R}^{q}, C∈Mp×q(R)C\in\mathcal{M}_{p\times q}(\mathbb{R}) and u,v∈Iu,v\in I. The integrals from uu to vv of the constant maps I→RqI\to\mathbb{R}^{q}, t↦bt\mapsto b, and I→Mp×q(R)I\to\mathcal{M}_{p\times q}(\mathbb{R}), t↦Ct\mapsto C, are defined, and

∫uvb dt=(v−u) b,∫uvC dt=(v−u) C.\int_{u}^{v}b\,dt=(v-u)\,b,\qquad\int_{u}^{v}C\,dt=(v-u)\,C .

Let u,v∈Iu,v\in I, L∈Mm×q(R)L\in\mathcal{M}_{m\times q}(\mathbb{R}), z∈Rqz\in\mathbb{R}^{q}, M∈Mm×p(R)M\in\mathcal{M}_{m\times p}(\mathbb{R}) and N∈Mq×n(R)N\in\mathcal{M}_{q\times n}(\mathbb{R}). If ∫uvx\int_{u}^{v}x is defined, then the following integrals are defined and

∫uvLx(t) dt=L∫uvx,∫uvz⋅x(t) dt=z⋅∫uvx.\int_{u}^{v}Lx(t)\,dt=L\int_{u}^{v}x,\qquad\int_{u}^{v}z\cdot x(t)\,dt=z\cdot\int_{u}^{v}x .

If ∫uvA\int_{u}^{v}A is defined, then the following integrals are defined and

∫uvA(t)z dt=(∫uvA)z,∫uvMA(t) dt=M∫uvA,∫uvA(t)N dt=(∫uvA)N,∫uv(MA(t))N dt=(M∫uvA)N.\int_{u}^{v}A(t)z\,dt=\Bigl(\int_{u}^{v}A\Bigr)z,\quad\int_{u}^{v}MA(t)\,dt=M\int_{u}^{v}A,\quad\int_{u}^{v}A(t)N\,dt=\Bigl(\int_{u}^{v}A\Bigr)N,\quad\int_{u}^{v}\bigl(MA(t)\bigr)N\,dt=\Bigl(M\int_{u}^{v}A\Bigr)N .

Let u,v∈Iu,v\in I. If ∫uvA\int_{u}^{v}A is defined, then ∫uvA(t)⊤dt\int_{u}^{v}A(t)^{\top}dt is defined and equals (∫uvA)⊤\bigl(\int_{u}^{v}A\bigr)^{\top}.

Let u,v∈Iu,v\in I with u≤vu\le v. If xx is continuous on II, then ∫uv∥x(t)∥ dt\int_{u}^{v}\lVert x(t)\rVert\,dt is defined and

∥∫uvx∥≤∫uv∥x(t)∥ dt.\Bigl\lVert\int_{u}^{v}x\Bigr\rVert\le\int_{u}^{v}\lVert x(t)\rVert\,dt .

If AA is continuous on II, then ∫uv∥A(t)∥ dt\int_{u}^{v}\lVert A(t)\rVert\,dt is defined and ∥∫uvA∥≤∫uv∥A(t)∥ dt\bigl\lVert\int_{u}^{v}A\bigr\rVert\le\int_{u}^{v}\lVert A(t)\rVert\,dt, with the operator norm.

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