Subfloat figure and text overlap in begin{figure}[H]












0














documentclass[sort&compress, 5p]{elsarticle}
usepackage{lineno}
journal{Journal of LaTeX Templates}
usepackage{subfig}
usepackage{pgf,tikz}
usetikzlibrary{shapes.geometric, arrows}
usepackage{multirow}
usepackage{float}
captionsetup[subfigure]{subrefformat=simple,labelformat=simple,listofformat=subsimple}
renewcommandthesubfigure{(alph{subfigure})}

begin{document}

%begin{figure}
%begin{figure*}
begin{figure}[H]
centering
subfloat[1]
{
includegraphics[height=2.40 in, width=2.35 in]{1.eps} label{a}
}
subfloat[2]
{
includegraphics[height=2.40 in, width=2.35 in]{2.eps} label{b}
}
subfloat[3]
{
includegraphics[height=2.40 in, width=2.35 in]{3.eps} label{c}
}\
subfloat[4]
{
includegraphics[height=2.40 in, width=2.35 in]{4.eps} label{d}
}
subfloat[5]
{
includegraphics[height=2.30 in, width=2.3 in]{5.eps} label{e}
}
subfloat[6]
{
includegraphics[height=2.30 in, width=2.3 in]{6.eps} label{f}
}
caption{Dynamic analysis iteration convergence properties: Approach 1. The energy tolerance is plotted against the time at every BGS iterations.} label{n-r_energy_tol_error_app1_dyn}
end{figure}
%end{figure*}

section{Dynamic analysis}
In this section, we demonstrate a comprehensive and systematic performances evaluation
of various numerical coupled algorithms based on accuracy and computational efficiency
to study the electric filed and structure interaction. The evaluated linear piezoelectric finite
element algorithms are 1) the monolithic coupling with Newmark’s time integration, 2) block
Jacobi partitioned iterative coupling with Newmark’s time integration, 3) block Gauss-Seidel
partitioned iterative coupling with Newmark’s time integration, 4) non iterative partitioned
coupling with central difference time integration. Using these algorithms, the static, dynamic
step responses and transient dynamic characteristics of piezoelectric bimorph actuator are
predicted accurately. The static and dynamic behaviors of the model from numerical and
analytic results are compared with each other. It is shown from these results that the numerical
analysis using the proposed algorithms takes into account the interaction of the structure-electric
field of the piezoelectric actuator accurately. The performances of the proposed algorithms
have been depicted in the present simulation results. The performances of these finite element
coupled algorithms are evaluated based on the accuracy of the solution and the computational
cost for piezoelectric bimorph actuators without metal shim, bimorph actuators with metal shim
(triple layer actuator), and surface acoustic wave devices. Their transient dynamic responses
are demonstrated together with the static and steady-state responses.

Here we present the numerical results obtained using the proposed finite element coupled
algorithms for piezoelectric bimorph actuator problems. These piezoelectric bimorph actuators
have a very wide area of applications and recently they have are used to actuate the insect-scale
robots [15, 17]. The piezoelectric bimorph actuators consist of a double layer of piezoelectric ceramic joined together over their long surfaces. Usually, a metal shim is attached between the two
piezoelectric ceramic in-order to enhance the reliability and mechanical strength. This type of
the piezoelectric bimorph actuator is called as bimorph actuators with metal shim or triple layer
actuator [22]. The classification of piezoelectric bimorph actuators are depicted in Fig. 2.9.
In general, two types of electrical connections are practically used in the configuration of
the bimorph actuator shown in Fig. 2.10. One is a series connection, where the piezoelectric
layers have opposite polarization directions, and an electric field is applied across the thickness
of the bimorph as shown in Figs. 2.10(a) and 2.10(c). The second type of connection is a
parallel connection, where the two piezoelectric ceramic layers have a polarization in the same
directions, and the electric field is applied across each individual layer with opposite polarity as
shown in Figs. 2.10(b) and 2.10(d). Due to the symmetrical structure, in both the case when an
electric field is applied to the piezoelectric layers, the induced electric forces in the upper half
thickness is canceled by that of the lower half thickness. Hence, for the given configurations in
Fig. 2.10 the upper piezoelectric layer contracts and lower piezoelectric layer expands, resulting
in a pure bending in the upward direction [22, 23]. Length, width and thickness directions of
the bimorph actuator are assigned as X , Y , and Z axes, respectively. Directional parameters of
end{document}


enter image description here



Dear Members,
In this latex code I used begin{figure}[H] to positioning the figure. It seems that the text and the figure overlap. Also, I tried with begin{figure*} and they do not overlap each other. However, begin{figure*} leave blank space after the figure. How can I use the left space after the figure in the same page. Thank you very much.










share|improve this question





























    0














    documentclass[sort&compress, 5p]{elsarticle}
    usepackage{lineno}
    journal{Journal of LaTeX Templates}
    usepackage{subfig}
    usepackage{pgf,tikz}
    usetikzlibrary{shapes.geometric, arrows}
    usepackage{multirow}
    usepackage{float}
    captionsetup[subfigure]{subrefformat=simple,labelformat=simple,listofformat=subsimple}
    renewcommandthesubfigure{(alph{subfigure})}

    begin{document}

    %begin{figure}
    %begin{figure*}
    begin{figure}[H]
    centering
    subfloat[1]
    {
    includegraphics[height=2.40 in, width=2.35 in]{1.eps} label{a}
    }
    subfloat[2]
    {
    includegraphics[height=2.40 in, width=2.35 in]{2.eps} label{b}
    }
    subfloat[3]
    {
    includegraphics[height=2.40 in, width=2.35 in]{3.eps} label{c}
    }\
    subfloat[4]
    {
    includegraphics[height=2.40 in, width=2.35 in]{4.eps} label{d}
    }
    subfloat[5]
    {
    includegraphics[height=2.30 in, width=2.3 in]{5.eps} label{e}
    }
    subfloat[6]
    {
    includegraphics[height=2.30 in, width=2.3 in]{6.eps} label{f}
    }
    caption{Dynamic analysis iteration convergence properties: Approach 1. The energy tolerance is plotted against the time at every BGS iterations.} label{n-r_energy_tol_error_app1_dyn}
    end{figure}
    %end{figure*}

    section{Dynamic analysis}
    In this section, we demonstrate a comprehensive and systematic performances evaluation
    of various numerical coupled algorithms based on accuracy and computational efficiency
    to study the electric filed and structure interaction. The evaluated linear piezoelectric finite
    element algorithms are 1) the monolithic coupling with Newmark’s time integration, 2) block
    Jacobi partitioned iterative coupling with Newmark’s time integration, 3) block Gauss-Seidel
    partitioned iterative coupling with Newmark’s time integration, 4) non iterative partitioned
    coupling with central difference time integration. Using these algorithms, the static, dynamic
    step responses and transient dynamic characteristics of piezoelectric bimorph actuator are
    predicted accurately. The static and dynamic behaviors of the model from numerical and
    analytic results are compared with each other. It is shown from these results that the numerical
    analysis using the proposed algorithms takes into account the interaction of the structure-electric
    field of the piezoelectric actuator accurately. The performances of the proposed algorithms
    have been depicted in the present simulation results. The performances of these finite element
    coupled algorithms are evaluated based on the accuracy of the solution and the computational
    cost for piezoelectric bimorph actuators without metal shim, bimorph actuators with metal shim
    (triple layer actuator), and surface acoustic wave devices. Their transient dynamic responses
    are demonstrated together with the static and steady-state responses.

    Here we present the numerical results obtained using the proposed finite element coupled
    algorithms for piezoelectric bimorph actuator problems. These piezoelectric bimorph actuators
    have a very wide area of applications and recently they have are used to actuate the insect-scale
    robots [15, 17]. The piezoelectric bimorph actuators consist of a double layer of piezoelectric ceramic joined together over their long surfaces. Usually, a metal shim is attached between the two
    piezoelectric ceramic in-order to enhance the reliability and mechanical strength. This type of
    the piezoelectric bimorph actuator is called as bimorph actuators with metal shim or triple layer
    actuator [22]. The classification of piezoelectric bimorph actuators are depicted in Fig. 2.9.
    In general, two types of electrical connections are practically used in the configuration of
    the bimorph actuator shown in Fig. 2.10. One is a series connection, where the piezoelectric
    layers have opposite polarization directions, and an electric field is applied across the thickness
    of the bimorph as shown in Figs. 2.10(a) and 2.10(c). The second type of connection is a
    parallel connection, where the two piezoelectric ceramic layers have a polarization in the same
    directions, and the electric field is applied across each individual layer with opposite polarity as
    shown in Figs. 2.10(b) and 2.10(d). Due to the symmetrical structure, in both the case when an
    electric field is applied to the piezoelectric layers, the induced electric forces in the upper half
    thickness is canceled by that of the lower half thickness. Hence, for the given configurations in
    Fig. 2.10 the upper piezoelectric layer contracts and lower piezoelectric layer expands, resulting
    in a pure bending in the upward direction [22, 23]. Length, width and thickness directions of
    the bimorph actuator are assigned as X , Y , and Z axes, respectively. Directional parameters of
    end{document}


    enter image description here



    Dear Members,
    In this latex code I used begin{figure}[H] to positioning the figure. It seems that the text and the figure overlap. Also, I tried with begin{figure*} and they do not overlap each other. However, begin{figure*} leave blank space after the figure. How can I use the left space after the figure in the same page. Thank you very much.










    share|improve this question



























      0












      0








      0


      1





      documentclass[sort&compress, 5p]{elsarticle}
      usepackage{lineno}
      journal{Journal of LaTeX Templates}
      usepackage{subfig}
      usepackage{pgf,tikz}
      usetikzlibrary{shapes.geometric, arrows}
      usepackage{multirow}
      usepackage{float}
      captionsetup[subfigure]{subrefformat=simple,labelformat=simple,listofformat=subsimple}
      renewcommandthesubfigure{(alph{subfigure})}

      begin{document}

      %begin{figure}
      %begin{figure*}
      begin{figure}[H]
      centering
      subfloat[1]
      {
      includegraphics[height=2.40 in, width=2.35 in]{1.eps} label{a}
      }
      subfloat[2]
      {
      includegraphics[height=2.40 in, width=2.35 in]{2.eps} label{b}
      }
      subfloat[3]
      {
      includegraphics[height=2.40 in, width=2.35 in]{3.eps} label{c}
      }\
      subfloat[4]
      {
      includegraphics[height=2.40 in, width=2.35 in]{4.eps} label{d}
      }
      subfloat[5]
      {
      includegraphics[height=2.30 in, width=2.3 in]{5.eps} label{e}
      }
      subfloat[6]
      {
      includegraphics[height=2.30 in, width=2.3 in]{6.eps} label{f}
      }
      caption{Dynamic analysis iteration convergence properties: Approach 1. The energy tolerance is plotted against the time at every BGS iterations.} label{n-r_energy_tol_error_app1_dyn}
      end{figure}
      %end{figure*}

      section{Dynamic analysis}
      In this section, we demonstrate a comprehensive and systematic performances evaluation
      of various numerical coupled algorithms based on accuracy and computational efficiency
      to study the electric filed and structure interaction. The evaluated linear piezoelectric finite
      element algorithms are 1) the monolithic coupling with Newmark’s time integration, 2) block
      Jacobi partitioned iterative coupling with Newmark’s time integration, 3) block Gauss-Seidel
      partitioned iterative coupling with Newmark’s time integration, 4) non iterative partitioned
      coupling with central difference time integration. Using these algorithms, the static, dynamic
      step responses and transient dynamic characteristics of piezoelectric bimorph actuator are
      predicted accurately. The static and dynamic behaviors of the model from numerical and
      analytic results are compared with each other. It is shown from these results that the numerical
      analysis using the proposed algorithms takes into account the interaction of the structure-electric
      field of the piezoelectric actuator accurately. The performances of the proposed algorithms
      have been depicted in the present simulation results. The performances of these finite element
      coupled algorithms are evaluated based on the accuracy of the solution and the computational
      cost for piezoelectric bimorph actuators without metal shim, bimorph actuators with metal shim
      (triple layer actuator), and surface acoustic wave devices. Their transient dynamic responses
      are demonstrated together with the static and steady-state responses.

      Here we present the numerical results obtained using the proposed finite element coupled
      algorithms for piezoelectric bimorph actuator problems. These piezoelectric bimorph actuators
      have a very wide area of applications and recently they have are used to actuate the insect-scale
      robots [15, 17]. The piezoelectric bimorph actuators consist of a double layer of piezoelectric ceramic joined together over their long surfaces. Usually, a metal shim is attached between the two
      piezoelectric ceramic in-order to enhance the reliability and mechanical strength. This type of
      the piezoelectric bimorph actuator is called as bimorph actuators with metal shim or triple layer
      actuator [22]. The classification of piezoelectric bimorph actuators are depicted in Fig. 2.9.
      In general, two types of electrical connections are practically used in the configuration of
      the bimorph actuator shown in Fig. 2.10. One is a series connection, where the piezoelectric
      layers have opposite polarization directions, and an electric field is applied across the thickness
      of the bimorph as shown in Figs. 2.10(a) and 2.10(c). The second type of connection is a
      parallel connection, where the two piezoelectric ceramic layers have a polarization in the same
      directions, and the electric field is applied across each individual layer with opposite polarity as
      shown in Figs. 2.10(b) and 2.10(d). Due to the symmetrical structure, in both the case when an
      electric field is applied to the piezoelectric layers, the induced electric forces in the upper half
      thickness is canceled by that of the lower half thickness. Hence, for the given configurations in
      Fig. 2.10 the upper piezoelectric layer contracts and lower piezoelectric layer expands, resulting
      in a pure bending in the upward direction [22, 23]. Length, width and thickness directions of
      the bimorph actuator are assigned as X , Y , and Z axes, respectively. Directional parameters of
      end{document}


      enter image description here



      Dear Members,
      In this latex code I used begin{figure}[H] to positioning the figure. It seems that the text and the figure overlap. Also, I tried with begin{figure*} and they do not overlap each other. However, begin{figure*} leave blank space after the figure. How can I use the left space after the figure in the same page. Thank you very much.










      share|improve this question















      documentclass[sort&compress, 5p]{elsarticle}
      usepackage{lineno}
      journal{Journal of LaTeX Templates}
      usepackage{subfig}
      usepackage{pgf,tikz}
      usetikzlibrary{shapes.geometric, arrows}
      usepackage{multirow}
      usepackage{float}
      captionsetup[subfigure]{subrefformat=simple,labelformat=simple,listofformat=subsimple}
      renewcommandthesubfigure{(alph{subfigure})}

      begin{document}

      %begin{figure}
      %begin{figure*}
      begin{figure}[H]
      centering
      subfloat[1]
      {
      includegraphics[height=2.40 in, width=2.35 in]{1.eps} label{a}
      }
      subfloat[2]
      {
      includegraphics[height=2.40 in, width=2.35 in]{2.eps} label{b}
      }
      subfloat[3]
      {
      includegraphics[height=2.40 in, width=2.35 in]{3.eps} label{c}
      }\
      subfloat[4]
      {
      includegraphics[height=2.40 in, width=2.35 in]{4.eps} label{d}
      }
      subfloat[5]
      {
      includegraphics[height=2.30 in, width=2.3 in]{5.eps} label{e}
      }
      subfloat[6]
      {
      includegraphics[height=2.30 in, width=2.3 in]{6.eps} label{f}
      }
      caption{Dynamic analysis iteration convergence properties: Approach 1. The energy tolerance is plotted against the time at every BGS iterations.} label{n-r_energy_tol_error_app1_dyn}
      end{figure}
      %end{figure*}

      section{Dynamic analysis}
      In this section, we demonstrate a comprehensive and systematic performances evaluation
      of various numerical coupled algorithms based on accuracy and computational efficiency
      to study the electric filed and structure interaction. The evaluated linear piezoelectric finite
      element algorithms are 1) the monolithic coupling with Newmark’s time integration, 2) block
      Jacobi partitioned iterative coupling with Newmark’s time integration, 3) block Gauss-Seidel
      partitioned iterative coupling with Newmark’s time integration, 4) non iterative partitioned
      coupling with central difference time integration. Using these algorithms, the static, dynamic
      step responses and transient dynamic characteristics of piezoelectric bimorph actuator are
      predicted accurately. The static and dynamic behaviors of the model from numerical and
      analytic results are compared with each other. It is shown from these results that the numerical
      analysis using the proposed algorithms takes into account the interaction of the structure-electric
      field of the piezoelectric actuator accurately. The performances of the proposed algorithms
      have been depicted in the present simulation results. The performances of these finite element
      coupled algorithms are evaluated based on the accuracy of the solution and the computational
      cost for piezoelectric bimorph actuators without metal shim, bimorph actuators with metal shim
      (triple layer actuator), and surface acoustic wave devices. Their transient dynamic responses
      are demonstrated together with the static and steady-state responses.

      Here we present the numerical results obtained using the proposed finite element coupled
      algorithms for piezoelectric bimorph actuator problems. These piezoelectric bimorph actuators
      have a very wide area of applications and recently they have are used to actuate the insect-scale
      robots [15, 17]. The piezoelectric bimorph actuators consist of a double layer of piezoelectric ceramic joined together over their long surfaces. Usually, a metal shim is attached between the two
      piezoelectric ceramic in-order to enhance the reliability and mechanical strength. This type of
      the piezoelectric bimorph actuator is called as bimorph actuators with metal shim or triple layer
      actuator [22]. The classification of piezoelectric bimorph actuators are depicted in Fig. 2.9.
      In general, two types of electrical connections are practically used in the configuration of
      the bimorph actuator shown in Fig. 2.10. One is a series connection, where the piezoelectric
      layers have opposite polarization directions, and an electric field is applied across the thickness
      of the bimorph as shown in Figs. 2.10(a) and 2.10(c). The second type of connection is a
      parallel connection, where the two piezoelectric ceramic layers have a polarization in the same
      directions, and the electric field is applied across each individual layer with opposite polarity as
      shown in Figs. 2.10(b) and 2.10(d). Due to the symmetrical structure, in both the case when an
      electric field is applied to the piezoelectric layers, the induced electric forces in the upper half
      thickness is canceled by that of the lower half thickness. Hence, for the given configurations in
      Fig. 2.10 the upper piezoelectric layer contracts and lower piezoelectric layer expands, resulting
      in a pure bending in the upward direction [22, 23]. Length, width and thickness directions of
      the bimorph actuator are assigned as X , Y , and Z axes, respectively. Directional parameters of
      end{document}


      enter image description here



      Dear Members,
      In this latex code I used begin{figure}[H] to positioning the figure. It seems that the text and the figure overlap. Also, I tried with begin{figure*} and they do not overlap each other. However, begin{figure*} leave blank space after the figure. How can I use the left space after the figure in the same page. Thank you very much.







      floats positioning subfloats overlap






      share|improve this question















      share|improve this question













      share|improve this question




      share|improve this question








      edited 16 mins ago







      Prakash

















      asked 23 mins ago









      PrakashPrakash

      777




      777






















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