Navigation: **1. Exact, conservative and closed forms** | 2. Locally exact forms and singular homology | 3. Applications to complex analysis

The line integral is a useful tool for working with vector fields on \(\mathbb{R}^n\), (co)vector fields on manifolds, and complex differentiable functions. However, it is often unclear how these different versions of the line integral are related to each other. In the next few posts, I will be presenting a very general form of the line integral along with the standard theorems and some basic applications. Familiarity with the Fréchet derivative is assumed.

Let \(E,F\) be (real or complex) Banach spaces and let \(U\subseteq E\) be an open set. We define a **form on \(U\)** to be a continuous map \(\omega:U\to L(E,F)\), where \(L(E,F)\) is the space of continuous linear maps from \(E\) to \(F\). A **path in \(U\)** is a continuous map \(\gamma:[a,b]\to U\). If \(\gamma(a)=\gamma(b)\) then we say that \(\gamma\) is a **closed path**. We say that a continuous map \(\gamma:[a,b]\to U\) is a **curve** if there is a partition \(a=a_0 < \cdots < a_k=b\) of \([a,b]\) such that \(\gamma|_{[a_{i-1},a_i]}\) is a continuously differentiable path for each \(i\). If \(\gamma(a)=\gamma(b)\) then we say that \(\gamma\) is a **closed curve**.

If \(\gamma:[a,b]\to U\) is a \(C^1\) path and \(\omega\) is a form on \(U\), we define the **(line) integral of \(\omega\) along \(\gamma\)** by $$

\int_\gamma \omega = \int_\gamma \omega(x)\,dx = \int_a^b \omega(\gamma(t))\gamma'(t)\,dt.

$$ (Note that \(\omega(\gamma(t))\) is a linear map from \(E\) to \(F\), and \(\gamma'(t)\in E\) since we are identifying \(\gamma'(t)\) with \(D\gamma(t)(1)\).) If \(\gamma\) is a curve with partition \(\{a_0,\dots,a_k\}\), we define the integral of \(\omega\) along \(\gamma\) by $$

\int_\gamma \omega = \int_\gamma \omega(x)\,dx = \sum_{i=1}^k \int_{\gamma|_{[a_{i-1},a_i]}} \omega.

$$

**Theorem 1** (Properties of line integrals). *Let \(\gamma:[a,b]\to U\) be a curve and let \(\omega,\eta\) be forms on \(U\).*

*For any scalars \(a,b\), $$\int_\gamma (a\omega+b\eta)=a\int_\gamma \omega+b\int_\gamma \eta.$$**For any Banach space \(G\) and any continuous linear map \(f:F\to G\), $$\int_\gamma f\omega = f\left(\int_\gamma \omega\right),$$ where \(f\omega:U\to L(E,G)\) is the form defined by \((f\omega)(x)u=f(\omega(x)u)\).**If \(\gamma\) is constant then $$\int_\gamma \omega = 0.$$**If \(\gamma_1=\gamma|_{[a,c]}\) and \(\gamma_2=\gamma|_{[c,b]}\) where \(a < c < b\) then $$\int_\gamma \omega = \int_{\gamma_1} \omega + \int_{\gamma_2} \omega.$$**If \(\varphi:[c,d]\to [a,b]\) is a continuously differentiable function with \(\varphi(c)=a\) and \(\varphi(d)=b\) then $$\int_{\gamma\circ\varphi} \omega = \int_\gamma \omega.$$ If \(\varphi(c)=b\) and \(\varphi(d)=a\) (i.e. \(\varphi\) is decreasing) then $$\int_{\gamma\circ\varphi} \omega = -\int_\gamma \omega.$$**We have $$\left\vert\int_\gamma \omega\right\vert \le L(\gamma) \sup_{t\in[a,b]} |\omega(\gamma(t))|,$$ where \(L(\gamma)\) is the length of \(\gamma\) defined by $$L(\gamma)=\sum_{i=1}^k\int_{a_{i-1}}^{a_i} |\gamma'(t)|\,dt.$$**If \(\{\omega_n\}\) is a sequence of forms on \(U\) converging uniformly to a form \(\omega\), then $$\int_\gamma \omega = \lim_{n\to\infty}\int_\gamma \omega_n.$$*

*Proof.* By linearity, we can assume that \(\gamma\) is a \(C^1\) path. For (2), we have \begin{align}

\int_\gamma f\omega &= \int_a^b f(\omega(\gamma(t))\gamma'(t))\,dt \\

&= f\left(\int_a^b \omega(\gamma(t))\gamma'(t)\,dt\right) \\

&= f\left(\int_\gamma \omega\right)

\end{align} using one of the basic properties of the regulated integral or Bochner integral. For (4), we have \begin{align}

\int_{\gamma\circ\varphi} \omega &= \int_c^d \omega((\gamma\circ\varphi)(t))(\gamma\circ\varphi)'(t)\,dt \\

&= \int_c^d \omega(\gamma(\varphi(t)))\gamma'(\varphi(t))\varphi'(t)\,dt \\

&= \int_a^b \omega(\gamma(t))\gamma'(t)\,dt \\

&= \int_\gamma \omega

\end{align} by the change of variables formula. For (5), we have \begin{align}

\left\vert\int_\gamma \omega\right\vert &= \left\vert\int_a^b \omega(\gamma(t))\gamma'(t)\,dt\right\vert \\

&\le \int_a^b |\omega(\gamma(t))||\gamma'(t)|\,dt \\

&\le L(\gamma) \sup_{t\in[a,b]} |\omega(\gamma(t))|.

\end{align} For (6), we have \begin{align}

\left\vert\int_\gamma \omega_n – \int_\gamma \omega\right\vert &= \left\vert\int_\gamma (\omega_n-\omega)\right\vert \\

&\le L(\gamma) \sup_{t\in[a,b]} |(\omega_n-\omega)(\gamma(t))| \\

&\to 0

\end{align} as \(n\to\infty\). \(\square\)

**Example** (Line integrals in \(\mathbb{R}^n\)). If \(U\subseteq\mathbb{R}^n\) is an open set and \(F:U\to\mathbb{R}^n\) is a vector field, then its **associated form** \(\omega_F:U\to L(\mathbb{R}^n,\mathbb{R})\) is given by $$\omega_F(x)v=F(x)\cdot v,$$ where \(\cdot\) is the usual dot product on \(\mathbb{R}^n\). We can then define $$\int_\gamma F \cdot dr = \int_\gamma \omega_F = \int_a^b F(\gamma(t)) \cdot \gamma'(t)\,dt$$ for any curve \(\gamma:[a,b]\to U\).

**Example** (Complex line integrals). If \(U\subseteq\mathbb{C}\) is an open set and \(f:U\to\mathbb{C}\) is continuous, then its **associated form** \(\omega_f:U\to L(\mathbb{C},\mathbb{C})\) is given by $$\omega_f(z)w=wf(z).$$ We can then define $$\int_\gamma f(z)\,dz = \int_\gamma \omega_f = \int_a^b f(\gamma(t))\gamma'(t)\,dt$$ for any curve \(\gamma:[a,b]\to U\). Later, we will examine this type of line integral more closely.

## Exact, conservative and closed forms

We have an important generalization of the fundamental theorem of calculus to line integrals.

**Theorem 2** (Fundamental theorem for line integrals). *Let \(f:U\to F\) be continuously differentiable and let \(\gamma:[a,b]\to U\) be a curve. Then $$\int_\gamma Df = f(\gamma(b))-f(\gamma(a)).$$*

*Proof.* First assume that \(\gamma\) is a \(C^1\) path. Then \begin{align}

\int_\gamma Df &= \int_a^b Df(\gamma(t))\gamma'(t)\,dt \\

&= \int_a^b (f\circ\gamma)'(t)\,dt \\

&= f(\gamma(b))-f(\gamma(a))

\end{align} by the fundamental theorem of calculus. If \(\gamma\) is a curve with partition \(\{a_0,\dots,a_k\}\) then $$

\int_\gamma Df = \sum_{i=1}^k [f(\gamma(a_k))-f(\gamma(a_{k-1}))] = f(\gamma(b))-f(\gamma(a)).

$$ \(\square\)

Note that in particular we have $$\int_\gamma Df = 0$$ for any closed curve \(\gamma\) in \(U\). If \(\omega\) is a form on \(U\), a function \(f:U\to F\) satisfying \(\omega=Df\) is called a **potential for \(\omega\)**. We say that a form \(\omega\) is **exact** if it has a potential function. Note that if \(U\) is connected then this result implies that \(f-g\) is constant if \(f,g\) are any two potentials for \(\omega\). If the integral of \(\omega\) along any closed curve is zero, then we say that \(\omega\) is **conservative**. It is easy to see that a form is conservative if and only if it is path-independent, in the sense that $$\int_\gamma \omega=\int_{\widetilde{\gamma}} \omega$$ whenever \(\gamma,\widetilde{\gamma}\) are curves with the same starting and ending points.

**Theorem 3.** *A form is conservative if and only if it is exact.*

*Proof.* Theorem 2 shows that every exact form is conservative, so it remains to show that every conservative form is exact. Let \(\omega\) be a conservative form on \(U\). We can assume that \(U\) is connected, for otherwise we can obtain a potential function \(f_\alpha\) on each component \(U_\alpha\) of \(U\) and define a potential \(f:U\to F\) for \(\omega\) by setting \(f|_{U_\alpha}=f_\alpha\). Since \(\omega\) is path-independent, for any two points \(x,y\in U\) we can define $$\int_x^y \omega=\int_\gamma \omega$$ where \(\gamma\) is any curve from \(x\) to \(y\). Choose some \(x_0\in U\) and let $$f(x)=\int_{x_0}^x \omega;$$ we want to show that \(\omega=Df\). Let \(x\in U\) and choose \(r > 0\) so that the open ball of radius \(r\) around \(x\) is contained in \(U\). For all \(|h| < r\) the straight line from \(x\) to \(x+h\) is contained in \(U\), so \begin{align}
\frac{1}{|h|} |f(x+h)-f(x)-\omega(x)h| &= \frac{1}{|h|}\left\vert\int_{x_0}^{x+h} \omega - \int_{x_0}^x \omega - \omega(x)h\right\vert \\
&= \frac{1}{|h|}\left\vert\int_x^{x+h} \omega - \omega(x)h\right\vert \\
&= \frac{1}{|h|}\left\vert\int_0^1 \omega(x+th)h\,dt-\int_0^1 \omega(x)h\,dt\right\vert \\
&= \frac{1}{|h|}\left\vert\left(\int_0^1 [\omega(x+th)-\omega(x)]\,dt\right)h\right\vert \\
&\le \sup_{t\in[0,1]} |\omega(x+th)-\omega(x)| \\
&\to 0
\end{align} as \(h\to 0\) since \(\omega\) is continuous. \(\square\)
If \(\omega\) is a differentiable form on \(U\), we say that \(\omega\) is **closed** if \(D\omega(x)\in L(E,E;F)\) is symmetric for every \(x\in U\). If \(\omega=Df\) for some \(C^2\) map \(f:U\to F\) then \(D\omega(x)=D^2 f(x)\) is always symmetric, so we have the following result:

**Theorem 4.** *Every exact \(C^1\) form is closed.* \(\square\)

The converse of Theorem 4 holds for certain kinds of sets. A set \(A\) in a vector space is **star-shaped** with respect to \(x_0\in A\) if the line segment from \(x_0\) to any \(x\in A\) is contained in \(A\).

**Theorem 5** (Poincaré lemma). *Let \(U\subseteq E\) be a star-shaped open set. Every closed \(C^1\) form on \(U\) is exact.*

*Proof.* Suppose that \(U\) is star-shaped with respect to some \(x_0\in U\). By translating \(U\), we can assume that \(x_0=0\). Let \(\omega\) be a closed form on \(U\). Define $$f(x)=\int_0^1 \omega(tx)x\,dt,$$ which is simply the integral of \(\omega\) along the straight line segment from \(0\) to \(x\). Using differentiation under the integral sign and the symmetry of \(D\omega(tx)\), \begin{align}

Df(x)u &= \int_0^1 [tD\omega(tx)(u,x)+\omega(tx)u]\,dt \\

&= \int_0^1 [tD\omega(tx)(x,u)+\omega(tx)u]\,dt \\

&= \left(\int_0^1 [tD\omega(tx)x+\omega(tx)]\,dt\right)u \\

&= \left(\int_0^1 \frac{d}{dt}(t\omega(tx))\,dt\right)u \\

&= \omega(x)u.

\end{align} \(\square\)

**Lemma 6.** *Let \(R=[a,b]\times[c,d]\) be a rectangle and let \(\omega\) be a closed (differentiable) form defined on an open subset of \(\mathbb{R}^2\) containing \(R\). Then $$\int_{\partial R} \omega=0,$$ where the integral is taken counterclockwise along the boundary of \(R\).*

*Proof.* First note that \(D(D\omega(x))(y)=D\omega(x)\) is symmetric for all \(y\in\mathbb{R}^2\), so the Poincaré lemma shows that \(D\omega(x)\) is exact for all \(x\in R\). Decompose \(R\) into the four rectangles \begin{align}

R_1 &= [a,\tfrac{b-a}{2}]\times[c,\tfrac{d-c}{2}], \\

R_2 &= [\tfrac{b-a}{2},b]\times[c,\tfrac{d-c}{2}], \\

R_3 &= [a,\tfrac{b-a}{2}]\times[\tfrac{d-c}{2},d], \\

R_4 &= [\tfrac{b-a}{2},b]\times[\tfrac{d-c}{2},d].

\end{align} Due to the orientations of \(\partial R_1,\dots,\partial R_4\), the inside boundaries cancel and we have $$

\int_{\partial R} \omega = \sum_{i=1}^4 \int_{\partial R_i} \omega \quad\mathrm{and}\quad \left\vert\int_{\partial R} \omega\right\vert \le \sum_{i=1}^4 \left\vert\int_{\partial R_i} \omega\right\vert,$$ so there is a rectangle \(R^{(1)}\) among \(R_1,\dots,R_4\) for which $$\left\vert\int_{\partial R^{(1)}} \omega\right\vert \ge \frac{1}{4}\left\vert\int_{\partial R} \omega\right\vert.$$ Replacing \(R\) with \(R^{(1)}\) in the above, we have a rectangle \(R^{(2)}\subseteq R^{(1)}\) such that $$\left\vert\int_{\partial R^{(2)}} \omega\right\vert \ge \frac{1}{4}\left\vert\int_{\partial R^{(1)}} \omega\right\vert.$$ Repeating this process, we obtain a sequence of rectangles $$R^{(1)}\supseteq R^{(2)}\supseteq \cdots$$ such that $$\left\vert\int_{\partial R^{(n+1)}} \omega\right\vert \ge \frac{1}{4}\left\vert\int_{\partial R^{(n)}} \omega\right\vert$$ for all \(n\). Therefore $$\left\vert\int_{\partial R^{(n)}} \omega\right\vert \ge \frac{1}{4^n}\left\vert\int_{\partial R} \omega\right\vert.$$ If \(L_0\) is the length of \(\partial R\) and \(L_n\) is the length of \(\partial R^{(n)}\), then \(L_n=L_0/2^n\), and if \(\operatorname{diam} R\) is the diameter of \(R\), then \(\operatorname{diam} R^{(n)} = (\operatorname{diam} R)/2^n\). Since every \(R^{(n)}\) is compact and \(\operatorname{diam}R^{(n)} \to 0\) as \(n\to\infty\), there is exactly one point $$x_0\in\bigcap_{n=1}^\infty R^{(n)}.$$ Since \(\omega\) is differentiable at \(x_0\), there exists a neighborhood \(U\) of \(x_0\) such that $$\omega(x)=\omega(x_0)+D\omega(x_0)(x-x_0)+\theta(x-x_0)$$ for every \(x\in U\), where \(\theta\) is a continuous function into \(L(E,F)\) satisfying $$\lim_{x\to x_0} \frac{\theta(x-x_0)}{|x-x_0|} = 0.\tag{*}$$ (This follows directly from the definition of the derivative.) For sufficiently large \(n\) we have \(R^{(n)}\subseteq U\) and \begin{align}

\int_{\partial R^{(n)}} \omega &= \int_{\partial R^{(n)}} \omega(x_0)\,dx + \int_{\partial R^{(n)}} D\omega(x_0)(x-x_0)\,dx + \int_{\partial R^{(n)}} \theta(x-x_0)\,dx \\

&= \int_{\partial R^{(n)}} [\omega(x_0)-D\omega(x_0)x_0]\,dx + \int_{\partial R^{(n)}} D\omega(x_0) + \int_{\partial R^{(n)}} \theta(x-x_0)\,dx \\

&= \int_{\partial R^{(n)}} \theta(x-x_0)\,dx

\end{align} since \(x\mapsto [\omega(x_0)-D\omega(x_0)x_0]x\) is a primitive for the constant form \(\omega(x_0)-D\omega(x_0)x_0\) and \(D\omega(x_0)\) is exact. Therefore \begin{align}

\left\vert\int_{\partial R} \omega\right\vert &\le 4^n \left\vert\int_{\partial R^{(n)}} \omega\right\vert \\

&\le 4^n L_n \sup_{x\in R^{(n)}} |\theta(x-x_0)| \\

&\le 4^n L_n (\operatorname{diam} R^{(n)}) \sup_{x\in R^{(n)}\setminus\{x_0\}} \frac{|\theta(x-x_0)|}{|x-x_0|} \\

&\le L_0 (\operatorname{diam} R) \sup_{x\in R^{(n)}\setminus\{x_0\}} \frac{|\theta(x-x_0)|}{|x-x_0|} \\

&\to 0

\end{align} as \(n\to\infty\) by (*). \(\square\)

**Theorem 7** (Morera’s theorem). *If \(\omega\) is a form on a disc $$U=\{x\in\mathbb{R}^2:|x-x_0| < r\}$$ and $$\int_{\partial R} \omega = 0$$ for every rectangle \(R\) contained in \(U\), then \(\omega\) is exact.*

*Proof.* Define $$f(x)=\int_{x_0}^x \omega,$$ where the integral is taken along the sides of a rectangle whose opposite vertices are \(x_0\) are \(x\). By considering an appropriate rectangle we have $$f(x+h)-f(x)=\int_x^{x+h} \omega,$$ so we can use the argument in Theorem 3 to show that \(\omega=Df\). \(\square\)

**Corollary 8** (Goursat’s theorem). *If \(\omega\) is a closed (differentiable) form on a disc $$U=\{x\in\mathbb{R}^2:|x-x_0| < r\},$$ then \(\omega\) is exact.*

*Proof.* Apply Lemma 6 and Theorem 7. \(\square\)

A closed form \(\omega\) on \(U\) is said to be **locally exact** if for every \(x\in U\) there is a neighborhood \(V\subseteq U\) of \(x\) on which \(\omega\) is exact. The Poincaré lemma shows that every closed \(C^1\) form on an open subset of \(E\) is locally exact, and Corollary 8 shows that every closed form (not necessarily of class \(C^1\)) on an open subset of \(\mathbb{R}^2\) is locally exact. This latter result is fundamental to complex analysis.

Next time we will see why locally exact forms are important, and how we can interpret line integrals in the framework of singular homology.

Navigation: **1. Exact, conservative and closed forms** | 2. Locally exact forms and singular homology | 3. Applications to complex analysis

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LINE INTEGRALS FOR DIFFERENTIAL EQUATIONS AND LAGRANGIAN

Author Mircea Orasanu

ABSTRACT

We use cookies to enhance your experience on our website. By continuing to use our website, you are agreeing to our use of cookies. You can change your cookie settings at any time. Find out more They determine the observable uncertainties (variances) Δxij of the conjugated components of the position tensor rr of the complex system entity. Thus, one finds from Equation (38) the relation:

1 INTRODUCTION

According to Nottale’s works [6,7] and the previous Relations (36) and (37), the momentum stresses pipj, Equation (35), are generated by unobservable (first term) and observable (second term) stressesFor motions of complex system entities on Peano’s curves at the Compton scale, the uncertainty relations for the diagonal components, Equation (42), are formally similar to those of wave mechanics for the conjugate variables of momentum and position.

The application of the (fractal hydrodynamic) uncertainty relations to concrete complex systems and the evaluation of the state function are demonstrated in the following example. Using the solution for the test particle in the spherically symmetric Coulomb or Newton fields together with the method from where a are specific Coulomb’s or Newton’s lengths and n, l are the standard quantum numbers (n is the principal quantum number and l is the orbital quantum numbers).

According to our previous relations, for the r components of the dynamical variables of the test particle in the spherically symmetric Coulomb or Newton field. these appear in THESIS ( TEZA Author Horia Orasanu )

Dinamica Lagrangiană este capabilă sa opereze cu constrangeri dependente de timp, constrangeri care efectueaza lucru mecanic real, insa nu si lucru mecanic virtual. Ne putem gandi la lucrul mec. virtual ca “un lucru mecanic care a uitat de timp”. Nu exista nici o diferenta intre cele doua tipuri de lucru mecanic atat timp cat se opereaza cu constrangeri dependente de timp. De asemenea in cazul in care caracteristicile materialelor sau ale punctelor materiale si ale

Solidelor pe langa faptul ca sunt positive ,fara sa fie posibile deplasari in cadrul unui solid pe

Rmit optimizari cu legaturi neolonome in vadrul corpului sau solidului

Un caz important al optimizarii legaturilor neolonome este acela al structurilor unde in calculi apar alca

Tuiri din materiale cu proprietatea vasco elastic corespunzatoare anumitor situatiiFurthermore, in the case of narrow entrances that are inaccessible to the robot, the dilation of the walls closes those entrances, diminishes the wave expansion area, and as a consequence reduces the computation time. In this way, the remaining poses define the three-dimensional free configuration space. This step is computed n times, n being the amount of different orientations of the robot for which the C-space is created. The larger value of n that is chosen, the smoother the trajectory that will be computed, since the step in between orientations will be smaller. At the same time, the larger the value of n, the greater the amount of computation time that is needed for this step. An example of the output of this step can be seen in Figure 2, in which the third dimension is the orientation of the robot and n =20. The orientations are repeated above and below the calculated values in order to permit manoeuvres.

References

1. Bar-Yam, Y. Dynamics of Complex Systems; Addison-Wesley Publishing Company: Reading, MA, USA, 1997. [Google Scholar]

2. Mitchell, M. Complexity: A Guided Tour; Oxford University Press: Oxford, UK, 2009. [Google Scholar]

3. Bennett, C.H. How to define complexity in physics, and why. Complex. Entropy Phys. Inf. 1990, 8, 137–148. [Google Scholar]

4. Winfree, A.T. The Geometry of Biological Time, 2nd ed.; Interdisciplinary Applied Mathematics (Book 12); Springer: New York, NY, USA, 2000. [Google Scholar]

5. Badii, R.; Politi, A. Complexity: Hierarchical Structure and Scaling in Physics; Cambridge University Press: Cambridge, UK, 1997. [Google Scholar]

6. Nottale, L. Fractal Space-Time and Microphysics: Towards A Theory of Scale Relativity; World Scientific: Singapore, Singapore, 1993. [Google Scholar]

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then here we must to see that are possible some methods as Mir . Orasan that to solved some interior problems associated movement in dynamical theory of material point subjected of the force F

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LAGRANGIAN OPERATOR AND INTEGRALS

ABSTRACT\

Even and Odd Signals and Spectra

If the signal is an even (or odd) function of time, its spectrum is an even (or odd) function of frequency: