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    A thermodynamic approach to ferromagnetism and phase transitions.

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    The paper provides a modelling of the magnetization curve and of the ferromagnetic–paramagnetic transition within a continuum thermodynamic setting. The general model of the nonlinear, time dependent behaviour of ferromagnetic materials is accomplished by regarding the magnetization vector as an internal variable, namely as a vector field whose time evolution is a constitutive equation subject to the requirements of the second law of thermodynamics. The exchange interaction of the magnetization is modelled through a dependence of the free energy on the magnetization gradient. Consistent with the non-simple character of the material, the second law allows for a non-zero extra-entropy flux. A general three-dimensional scheme is elaborated which seems to be new in the literature. The three-dimensional setting is then established for stationary and homogeneous fields thus finding the collinearity and the corresponding form of the magnetic susceptibility. The whole evolution problem for the temperature and the magnetization is provided so that temperature-induced transition processes are allowed. The model accounts also for the dependence of the saturation magnetization on the temperature. Also for the sake of comparison with the existing literature, the evolution equations for the direction and the intensity of magnetization are derived. Known models, such as those of Landau–Lifshitz and Gilbert, are recovered as particular cases of saturated bodies. Next, the model is made more specific so as to account in detail for the saturation, the residual or spontaneous magnetization and the coercive field. First, the classical potential, which traces back to Ginzburg, and the Weiss model are revisited. The corresponding lack of the saturation effect or the description via implicit relations are emphasized. Hence, a new potential, with a logarithmic dependence on the magnetization, is investigated which provides the residual magnetization and the coercive field in an explicit way and satisfies expected properties of the residual magnetization as a function of the temperature

    Equivalent histories, minimal state and initial value problem in viscoelasticity. Math. Methods Appl. Sci. 28 (2005), no. 2, 233--251.

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    References: 10 [-] Reference Citations: 0 Review Citations: 0 In the standard theory of viscoelasticity the constitutive equation for the stress is T(x,t)=G0(x)E(x,t)+int0inftyG(x,xi)Et(x,xi),dxitag1 T(x,t)=G_0(x)E(x,t)+int_0^infty G'( x,xi)E^t(x,xi),dxi tag1 where EE is the infinitesimal strain tensor, G(x,) G(x,·) is the relaxation function, defined by G(x,s)coloneqG0(x)int0sG(x,xi),dxi, G(x,s)coloneq G_0(x)-int_0^s G'(x,xi),dxi, and assumed to be such that Ginfty(x)=limstoinftyG(x,s)G_infty(x)=lim_{stoinfty} G(x,s) is positive definite, and Et(x,)E^t(x,·) is the history. The main idea of this paper is to replace (1) by T(x,t)=intt0tG(x,txi)widehatE(x,xi),dxi+It0(x,tt0)tag2 T(x,t)=int_{t_0}^t G(x,t-xi)widehat E( x,xi),dxi+I^{t_0}(x,t-t_0) tag2 where It0(x,tt0)I^{t_0}(x,t-t_0) denotes the contribution to T(x,t)T( x,t) by the stress at a previous time t0t_0. It follows that limttoinftyIt0(x,tt0)=Ginfty(x)E(x,t0)lim_{ttoinfty}I^{t_0}(x,t-t_0)=G_infty(x) E(x,t_0) and moreover It(x,tt0)I^t(x,t-t_0) has the operative meaning of the stress tensor at time tt once the solid is held at a constant strain since t0t_0, i.e., E(,xi)=E(,t0)E(·,xi)=E(·,t_0), xiin[t0,t)xiin[t_0,t). Representation (2) involves the relation function G(x,)G(x,·), which is required only to have a limit value GinftyG_infty. Then, the authors consider the following initial-boundary value problem: Lu=0textinOmegatimesBbbR++,tag3 Lu=0 text{ in } Omegatimes{Bbb R}^{++}, tag3 u=widehatutextonpartialOmegautimesBbbR+,,,u(0)=u0,dotu(0)=dotu0textinoverlineOmega,tag4 u=widehat u text{ on }partialOmega_utimes{Bbb R}^+,,, u(0)=u_0, dot u(0)=dot u_0 text{ in }overlineOmega, tag4 Tn=widehatttildeI0ntextonpartialOmegaTtimesBbbR+. Tn=widehat t-tilde I^0n text{ on }partialOmega_Ttimes{Bbb R}^+. Here partialOmegaucappartialOmegaT=varnothingpartialOmega_ucappartialOmega_T=varnothing, partialOmegaucuppartialOmegaT=partialOmega partialOmega_ucuppartialOmega_T=partialOmega, widehatuwidehat u and widehattwidehat t are known functions on the pertinent domain, and Lucoloneqrhoddotunabla(G0nablau+Gtimesnablau)rhof=0textinOmegatimesBbbR++,tag5 Lucoloneq rhoddot u-nabla·(G'_0nabla u+ Gtimesnabla u)-rho f=0 text{ in }Omegatimes{Bbb R}^{++},tag5 rhof(tau)=rhob(tau)+nablawidehatI0(tau),rho f(tau)=rho b(tau)+nablawidehat I^0(tau), the body force bb and tildeI0tilde I^0 are known on overlineOmegatimesBbbR++overlineOmegatimes{Bbb R}^{++}, and tildeIt(tau)=int0inftyG(tau+s)Et(s),ds,tag6 tilde I^t(tau)=int_0^infty G(tau+s)E^t(s),ds,tag6 (Gtimesnablau)(tau)=int0tauG(ts)nablau(s),ds.(G'timesnabla u)(tau)=int_0^tau G'(t-s)nabla u(s),ds. Using the variational approach they prove that the functional associated with (3)--(6) has a stationary point uinC2,2(OmegatimesBbbR+,V)uin C^{2,2}(Omegatimes{Bbb R}^+,V) if and only if uu is a solution to the mixed problem (3)--(4). Next, the authors consider a virtual-work type formulation which provides a weak form of the initial-value problem for the system of the dynamics of viscoelastic solids. Applying the Fourier transform to the initial-boundary value problem which represents the weak formulation of the problem rhodotv(t)=nablaint0tG(ttau)nablav(tau),dt+b(t)textinBbbRtimesBbbR+,tag7 rho dot v(t)=nabla·int_0^t G(t-tau)nabla v(tau),dt+b(t) text{ in }{Bbb R}times{Bbb R}^+, tag7 v(x,0)=0,v(x,t)partialOmega=0tag8 v(x,0)=0, v(x,t)|_{partialOmega}=0 tag8 where v(x,t)=dotu(x,t)v(x,t)=dot u(x,t), under some assumption about b(t)b(t) they prove that there exists a unique virtual-work solution of problem (7)--(8) in a certain class of functions

    Going Beyond Counting First Authors in Author Co-citation Analysis

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    The present study examines one of the fundamental aspects of author co-citation analysis (ACA) - the way co-citation counts are defined. Co-citation counting provides the data on which all subsequent statistical analyses and mappings are based, and we compare ACA results based on two different types of co-citation counting - the traditional type that only counts the first one among a cited work's authors on the one hand and a non-traditional type that takes into account the first 5 authors of a cited work on the other hand. Results indicate that the picture produced through this non-traditional author co-citation counting contains more coherent author groups and is therefore considerably clearer. However, this picture represents fewer specialties in the research field being studied than that produced through the traditional first-author co-citation counting when the same number of top-ranked authors is selected and analyzed. Reasons for these effects are discussed

    Variations on the Author

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    “Variations on the Author” discusses two of Eduardo Coutinho’s recent films (Um Dia na Vida, from 2010, and Últimas Conversas, posthumously released in 2015) and their contribution to the general question of documentary authorship. The director’s filmography is characterized by a consistent yet self-effacing form of authorial self-inscription: Coutinho often features as an interviewer that rather than express opinions propels discourses; an interviewer that is good at listening. This mode of self-inscription characterizes him as an author who is not expressive but who is nonetheless markedly present on the screen. In Um Dia na Vida, however, Coutinho is completely absent form the image, while Últimas Conversas, on the contrary, includes a confessional prologue that moves the director from the margins to the center of his films. This article examines the ways in which these works stand out in the filmography of a director who offers new insights into the notion of cinematic authorship

    Appropriate Similarity Measures for Author Cocitation Analysis

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    We provide a number of new insights into the methodological discussion about author cocitation analysis. We first argue that the use of the Pearson correlation for measuring the similarity between authors’ cocitation profiles is not very satisfactory. We then discuss what kind of similarity measures may be used as an alternative to the Pearson correlation. We consider three similarity measures in particular. One is the well-known cosine. The other two similarity measures have not been used before in the bibliometric literature. Finally, we show by means of an example that our findings have a high practical relevance.information science;Pearson correlation;cosine;similarity measure;author cocitation analysis
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