A Hydrodynamic Instability Is Used to Create Aesthetically Appealing Patterns in Painting
Events
Loading … Spinner

Mendeley | Further Information

{"title"=>"A hydrodynamic instability is used to create aesthetically appealing patterns in painting", "type"=>"journal", "authors"=>[{"first_name"=>"Sandra", "last_name"=>"Zetina", "scopus_author_id"=>"54382564200"}, {"first_name"=>"Francisco A.", "last_name"=>"Godínez", "scopus_author_id"=>"37099909800"}, {"first_name"=>"Roberto", "last_name"=>"Zenit", "scopus_author_id"=>"6701376832"}], "year"=>2015, "source"=>"PLoS ONE", "identifiers"=>{"issn"=>"19326203", "doi"=>"10.1371/journal.pone.0126135", "pmid"=>"25942586", "scopus"=>"2-s2.0-84929119277", "pui"=>"604276084", "sgr"=>"84929119277"}, "id"=>"30fe9f28-7fb6-36de-b393-94191eec0503", "abstract"=>"Painters often acquire a deep empirical knowledge of the way in which paints and inks behave. Through experimentation and practice, they can control the way in which fluids move and deform to create textures and images. David Alfaro Siqueiros, a recognized Mexican muralist, invented an accidental painting technique to create new and unexpected textures. By pouring layers of paint of different colors on a horizontal surface, the paints infiltrate into each other creating patterns of aesthetic value. In this investigation, we reproduce the technique in a controlled manner. We found that for the correct color combination, the dual viscous layer becomes Rayleigh-Taylor unstable: the density mismatch of the two color paints drives the formation of a spotted pattern. Experiments and a linear instability analysis were conducted to understand the properties of the process. We also argue that this flow configuration can be used to study the linear properties of this instability.", "link"=>"http://www.mendeley.com/research/hydrodynamic-instability-used-create-aesthetically-appealing-patterns-painting", "reader_count"=>13, "reader_count_by_academic_status"=>{"Unspecified"=>1, "Professor > Associate Professor"=>1, "Researcher"=>3, "Student > Ph. D. Student"=>2, "Student > Postgraduate"=>1, "Student > Master"=>2, "Other"=>1, "Professor"=>2}, "reader_count_by_user_role"=>{"Unspecified"=>1, "Professor > Associate Professor"=>1, "Researcher"=>3, "Student > Ph. D. Student"=>2, "Student > Postgraduate"=>1, "Student > Master"=>2, "Other"=>1, "Professor"=>2}, "reader_count_by_subject_area"=>{"Engineering"=>2, "Unspecified"=>1, "Environmental Science"=>1, "Agricultural and Biological Sciences"=>2, "Physics and Astronomy"=>4, "Chemical Engineering"=>1, "Psychology"=>1, "Computer Science"=>1}, "reader_count_by_subdiscipline"=>{"Engineering"=>{"Engineering"=>2}, "Physics and Astronomy"=>{"Physics and Astronomy"=>4}, "Psychology"=>{"Psychology"=>1}, "Agricultural and Biological Sciences"=>{"Agricultural and Biological Sciences"=>2}, "Computer Science"=>{"Computer Science"=>1}, "Unspecified"=>{"Unspecified"=>1}, "Environmental Science"=>{"Environmental Science"=>1}, "Chemical Engineering"=>{"Chemical Engineering"=>1}}, "reader_count_by_country"=>{"Austria"=>1, "Luxembourg"=>1, "Spain"=>1}, "group_count"=>0}

Scopus | Further Information

{"@_fa"=>"true", "link"=>[{"@_fa"=>"true", "@ref"=>"self", "@href"=>"https://api.elsevier.com/content/abstract/scopus_id/84929119277"}, {"@_fa"=>"true", "@ref"=>"author-affiliation", "@href"=>"https://api.elsevier.com/content/abstract/scopus_id/84929119277?field=author,affiliation"}, {"@_fa"=>"true", "@ref"=>"scopus", "@href"=>"https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84929119277&origin=inward"}, {"@_fa"=>"true", "@ref"=>"scopus-citedby", "@href"=>"https://www.scopus.com/inward/citedby.uri?partnerID=HzOxMe3b&scp=84929119277&origin=inward"}], "prism:url"=>"https://api.elsevier.com/content/abstract/scopus_id/84929119277", "dc:identifier"=>"SCOPUS_ID:84929119277", "eid"=>"2-s2.0-84929119277", "dc:title"=>"A hydrodynamic instability is used to create aesthetically appealing patterns in painting", "dc:creator"=>"Zetina S.", "prism:publicationName"=>"PLoS ONE", "prism:eIssn"=>"19326203", "prism:volume"=>"10", "prism:issueIdentifier"=>"5", "prism:pageRange"=>nil, "prism:coverDate"=>"2015-05-05", "prism:coverDisplayDate"=>"5 May 2015", "prism:doi"=>"10.1371/journal.pone.0126135", "citedby-count"=>"2", "affiliation"=>[{"@_fa"=>"true", "affilname"=>"Universidad Nacional Autonoma de Mexico", "affiliation-city"=>"Mexico City", "affiliation-country"=>"Mexico"}], "pubmed-id"=>"25942586", "prism:aggregationType"=>"Journal", "subtype"=>"ar", "subtypeDescription"=>"Article", "article-number"=>"e0126135", "source-id"=>"10600153309"}

Facebook

  • {"url"=>"http%3A%2F%2Fjournals.plos.org%2Fplosone%2Farticle%3Fid%3D10.1371%252Fjournal.pone.0126135", "share_count"=>14, "like_count"=>43, "comment_count"=>29, "click_count"=>0, "total_count"=>86}

Twitter

Counter

  • {"month"=>"5", "year"=>"2015", "pdf_views"=>"162", "xml_views"=>"8", "html_views"=>"1311"}
  • {"month"=>"6", "year"=>"2015", "pdf_views"=>"35", "xml_views"=>"1", "html_views"=>"206"}
  • {"month"=>"7", "year"=>"2015", "pdf_views"=>"33", "xml_views"=>"0", "html_views"=>"365"}
  • {"month"=>"8", "year"=>"2015", "pdf_views"=>"14", "xml_views"=>"0", "html_views"=>"270"}
  • {"month"=>"9", "year"=>"2015", "pdf_views"=>"22", "xml_views"=>"3", "html_views"=>"186"}
  • {"month"=>"10", "year"=>"2015", "pdf_views"=>"14", "xml_views"=>"0", "html_views"=>"262"}
  • {"month"=>"11", "year"=>"2015", "pdf_views"=>"11", "xml_views"=>"1", "html_views"=>"236"}
  • {"month"=>"12", "year"=>"2015", "pdf_views"=>"9", "xml_views"=>"0", "html_views"=>"261"}
  • {"month"=>"1", "year"=>"2016", "pdf_views"=>"7", "xml_views"=>"0", "html_views"=>"304"}
  • {"month"=>"2", "year"=>"2016", "pdf_views"=>"0", "xml_views"=>"0", "html_views"=>"240"}
  • {"month"=>"3", "year"=>"2016", "pdf_views"=>"12", "xml_views"=>"0", "html_views"=>"267"}
  • {"month"=>"4", "year"=>"2016", "pdf_views"=>"7", "xml_views"=>"0", "html_views"=>"311"}
  • {"month"=>"5", "year"=>"2016", "pdf_views"=>"7", "xml_views"=>"0", "html_views"=>"253"}
  • {"month"=>"6", "year"=>"2016", "pdf_views"=>"6", "xml_views"=>"0", "html_views"=>"264"}
  • {"month"=>"7", "year"=>"2016", "pdf_views"=>"23", "xml_views"=>"0", "html_views"=>"242"}
  • {"month"=>"8", "year"=>"2016", "pdf_views"=>"31", "xml_views"=>"0", "html_views"=>"337"}
  • {"month"=>"9", "year"=>"2016", "pdf_views"=>"24", "xml_views"=>"0", "html_views"=>"454"}
  • {"month"=>"10", "year"=>"2016", "pdf_views"=>"42", "xml_views"=>"0", "html_views"=>"747"}
  • {"month"=>"11", "year"=>"2016", "pdf_views"=>"69", "xml_views"=>"0", "html_views"=>"831"}
  • {"month"=>"12", "year"=>"2016", "pdf_views"=>"198", "xml_views"=>"0", "html_views"=>"941"}
  • {"month"=>"1", "year"=>"2017", "pdf_views"=>"305", "xml_views"=>"1", "html_views"=>"1026"}
  • {"month"=>"2", "year"=>"2017", "pdf_views"=>"293", "xml_views"=>"0", "html_views"=>"925"}
  • {"month"=>"3", "year"=>"2017", "pdf_views"=>"227", "xml_views"=>"0", "html_views"=>"844"}
  • {"month"=>"4", "year"=>"2017", "pdf_views"=>"225", "xml_views"=>"1", "html_views"=>"652"}
  • {"month"=>"5", "year"=>"2017", "pdf_views"=>"263", "xml_views"=>"0", "html_views"=>"622"}
  • {"month"=>"6", "year"=>"2017", "pdf_views"=>"326", "xml_views"=>"0", "html_views"=>"877"}
  • {"month"=>"7", "year"=>"2017", "pdf_views"=>"376", "xml_views"=>"0", "html_views"=>"748"}
  • {"month"=>"8", "year"=>"2017", "pdf_views"=>"275", "xml_views"=>"0", "html_views"=>"510"}

Figshare

  • {"files"=>["https://ndownloader.figshare.com/files/2052898"], "description"=>"<p>Image sequence of the preparation of the experiment.</p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404448, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g003", "stats"=>{"downloads"=>3, "page_views"=>8, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Image_sequence_of_the_preparation_of_the_experiment_/1404448", "title"=>"Image sequence of the preparation of the experiment.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052899"], "description"=>"<p>Radial extent is measured by the size of the liquid pool, <i>R</i><sub><i>n</i></sub> = <i>D</i>/2. The mean height is inferred from the initial volume, </p><p></p><p></p><p><mi>H</mi></p><p><mi>m</mi><mi>e</mi><mi>a</mi><mi>n</mi></p><p></p><mo>=</mo><mi>V</mi><mo>/</mo><mo stretchy=\"false\">(</mo><mi>π</mi><p><mi>R</mi><mi>n</mi><mn>2</mn></p><mo stretchy=\"false\">)</mo><p></p><p></p>. The Reynolds number is Re ≈ 10<sup>−4</sup>. The measurements are compared with the predictions of Huppert [<a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.ref020\" target=\"_blank\">20</a>].<p></p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404449, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g004", "stats"=>{"downloads"=>1, "page_views"=>10, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Measurement_of_the_spread_of_the_black_paint_/1404449", "title"=>"Measurement of the spread of the black paint.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052903"], "description"=>"<p>The time difference in between frames is 63 s. Time progresses from left to right and from top to bottom. The size of each image is 14.7 × 9.8 mm<sup>2</sup>. <i>At</i> = 0.05, with <i>H</i><sub>1</sub> = 2 mm and <i>H</i><sub>2</sub> = 1.2 mm. (See <a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.s001\" target=\"_blank\">S1 Movie</a> in Supporting Information section).</p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404453, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g005", "stats"=>{"downloads"=>2, "page_views"=>21, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Image_sequence_white_over_black_paint_/1404453", "title"=>"Image sequence, white over black paint.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052907"], "description"=>"<p><i>At</i> = 0.02, with <i>H</i><sub>1</sub> = 2 mm and <i>H</i><sub>2</sub> = 1.5 mm. The image size is approximately 14 × 9 mm<sup>2</sup>. For the experiments shown here, <i>Re</i> = 1.1 × 10<sup>−4</sup>, <i>At</i> = 0.03 and Π = 1.5 × 10<sup>−2</sup>.</p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404457, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g006", "stats"=>{"downloads"=>3, "page_views"=>31, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Final_pattern_yellow_paint_over_transparent_lacquer_/1404457", "title"=>"Final pattern, yellow paint over transparent lacquer.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052908"], "description"=>"<p>The horizontal dashed line shows the average of the measurement, <i>L</i><sub><i>c</i></sub>, for 230 < <i>t</i> < 300s. This measurements correspond to the images shown in <a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.g005\" target=\"_blank\">Fig 5</a>.</p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404458, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g007", "stats"=>{"downloads"=>0, "page_views"=>7, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Correlation_length_as_a_function_of_time_/1404458", "title"=>"Correlation length as a function of time.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052909"], "description"=>"<p>The solid black line shows the results considering the values in <a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.t001\" target=\"_blank\">Table 1</a> (<i>At</i> = 0.05). The dashed and dashed-dotted black lines show the influence of reducing the layer thickness: (− − −), <i>H</i><sub>1</sub> = 1 mm, <i>H</i><sub>2</sub> = 0.6 mm; (− ⋅ −), <i>H</i><sub>1</sub> = 0.4 mm, <i>H</i><sub>2</sub> = 0.2 mm. The red lines show the effect of changing the fluid viscosities, keeping the rest of the parameters fixed (layer thicknesses and densities). The red dashed line shows the prediction for smaller viscosities: <i>μ</i><sub>1</sub> = 5.79 Pa s, <i>μ</i><sub>2</sub> = 1.26 Pa s); the red dashed-dotted line shows the case for higher viscosities: <i>μ</i><sub>1</sub> = 23.14Pa s, <i>μ</i><sub>2</sub> = 5.04 Pa s). The blue lines show the effect of changing the density difference, keeping the rest of the parameters fixed. The blue dashed line shows the prediction for a smaller density difference (<i>At</i> = 0.02) produced by reducing the density of the top or bottom layer (<i>ρ</i><sub>1</sub> = 1002 kg/m<sup>3</sup>, <i>ρ</i><sub>2</sub> = 1050 kg/m<sup>3</sup>); the blue dashed dotted line corresponds also to a smaller density difference (<i>At</i> = 0.02) but by increasing the density of the bottom layer (<i>ρ</i><sub>1</sub> = 1050 kg/m<sup>3</sup>, <i>ρ</i><sub>2</sub> = 1110 kg/m<sup>3</sup>). The vertical gray line shows the experimental measurements of the mean blob size from <a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.g005\" target=\"_blank\">Fig 5</a>. Note that both <i>n</i> and <i>k</i> are shown in dimensionless form, considering, (<i>g</i><sup>2</sup><i>ρ</i><sub>1</sub>/<i>μ</i><sub>1</sub>)<sup>−1/3</sup> and </p><p></p><p></p><p></p><p><mo stretchy=\"false\">(</mo><mi>g</mi></p><p><mi>ρ</mi><mn>1</mn><mn>2</mn></p><mo>/</mo><p><mi>μ</mi><mn>1</mn><mn>2</mn></p><mo stretchy=\"false\">)</mo><p></p><p><mo>−</mo><mn>1</mn><mo>/</mo><mn>3</mn></p><p></p><p></p><p></p> respectively.<p></p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404459, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g008", "stats"=>{"downloads"=>2, "page_views"=>6, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Dispersion_relation_of_the_black_white_layer_/1404459", "title"=>"Dispersion relation of the black/white layer.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052911"], "description"=>"<p>Results shown for <i>At</i> = 0.05 and <i>H</i><sub>1</sub> = 2.0 mm and <i>H</i><sub>2</sub> = 1.2 mm. The continuous line shows the dispersion relation from considering the confined fluid layer; The dashed line shows the dispersion relation from a triple fluid layer, considering air properties for the upper most layer. The vertical gray line shows the experimental measurements of the mean blob size from <a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.g005\" target=\"_blank\">Fig 5</a>. The vertical dashed lines (blue and red) show the measurements of blob sizes from ‘Collective Suicide’ [<a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.ref014\" target=\"_blank\">14</a>] and ‘The Birth of Fascism’ [<a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.ref011\" target=\"_blank\">11</a>], (respectively). Note that both <i>n</i> and <i>k</i> are shown in dimensionless form, considering, (<i>g</i><sup>2</sup><i>ρ</i><sub>1</sub>/<i>μ</i><sub>1</sub>)<sup>−1/3</sup> and </p><p></p><p></p><p></p><p><mo stretchy=\"false\">(</mo><mi>g</mi></p><p><mi>ρ</mi><mn>1</mn><mn>2</mn></p><mo>/</mo><p><mi>μ</mi><mn>1</mn><mn>2</mn></p><mo stretchy=\"false\">)</mo><p></p><p><mo>−</mo><mn>1</mn><mo>/</mo><mn>3</mn></p><p></p><p></p><p></p> respectively.<p></p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404461, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g009", "stats"=>{"downloads"=>1, "page_views"=>18, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Dispersion_relation_of_the_black_white_layer_/1404461", "title"=>"Dispersion relation of the black/white layer.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052912"], "description"=>"<p>Properties of the fluids used: color, density, viscosity and initial layer thickness.</p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404462, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.t001", "stats"=>{"downloads"=>7, "page_views"=>14, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Properties_of_the_fluids_used_color_density_viscosity_and_initial_layer_thickness_/1404462", "title"=>"Properties of the fluids used: color, density, viscosity and initial layer thickness.", "pos_in_sequence"=>0, "defined_type"=>3, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052966", "https://ndownloader.figshare.com/files/2052968"], "description"=>"<div><p>Painters often acquire a deep empirical knowledge of the way in which paints and inks behave. Through experimentation and practice, they can control the way in which fluids move and deform to create textures and images. David Alfaro Siqueiros, a recognized Mexican muralist, invented an <i>accidental painting</i> technique to create new and unexpected textures. By pouring layers of paint of different colors on a horizontal surface, the paints infiltrate into each other creating patterns of aesthetic value. In this investigation, we reproduce the technique in a controlled manner. We found that for the correct color combination, the dual viscous layer becomes Rayleigh-Taylor unstable: the density mismatch of the two color paints drives the formation of a spotted pattern. Experiments and a linear instability analysis were conducted to understand the properties of the process. We also argue that this flow configuration can be used to study the linear properties of this instability.</p></div>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404499, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>["https://dx.doi.org/10.1371/journal.pone.0126135.s001", "https://dx.doi.org/10.1371/journal.pone.0126135.s002"], "stats"=>{"downloads"=>15, "page_views"=>44, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_A_Hydrodynamic_Instability_Is_Used_to_Create_Aesthetically_Appealing_Patterns_in_Painting_/1404499", "title"=>"A Hydrodynamic Instability Is Used to Create Aesthetically Appealing Patterns in Painting", "pos_in_sequence"=>0, "defined_type"=>4, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052883"], "description"=>"<p>Detail of ‘Collective Suicide’ [<a href=\"http://www.plosone.org/article/info:doi/10.1371/journal.pone.0126135#pone.0126135.ref014\" target=\"_blank\">14</a>], Approximate image size 16.2 x 16.0 cm<sup>2</sup>, Museum of Modern Art, New York (1936).</p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404445, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g001", "stats"=>{"downloads"=>3, "page_views"=>29, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_An_example_of_the_experimental_painting_technique_of_Siqueiros_/1404445", "title"=>"An example of the experimental painting technique of Siqueiros.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}
  • {"files"=>["https://ndownloader.figshare.com/files/2052884"], "description"=>"<p>Experimental setup.</p>", "links"=>[], "tags"=>["instability analysis", "Hydrodynamic Instability", "density mismatch", "Mexican muralist", "painting technique", "color combination", "fluids move", "flow configuration", "color paints drives", "David Alfaro Siqueiros", "pattern"], "article_id"=>1404446, "categories"=>["Biological Sciences", "Science Policy"], "users"=>["Sandra Zetina", "Francisco A. Godínez", "Roberto Zenit"], "doi"=>"https://dx.doi.org/10.1371/journal.pone.0126135.g002", "stats"=>{"downloads"=>4, "page_views"=>12, "likes"=>0}, "figshare_url"=>"https://figshare.com/articles/_Experimental_setup_/1404446", "title"=>"Experimental setup.", "pos_in_sequence"=>0, "defined_type"=>1, "published_date"=>"2015-05-05 03:01:03"}

PMC Usage Stats | Further Information

  • {"unique-ip"=>"15", "full-text"=>"15", "pdf"=>"7", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"1", "supp-data"=>"10", "cited-by"=>"0", "year"=>"2015", "month"=>"5"}
  • {"unique-ip"=>"16", "full-text"=>"14", "pdf"=>"7", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"12", "supp-data"=>"4", "cited-by"=>"0", "year"=>"2015", "month"=>"6"}
  • {"unique-ip"=>"17", "full-text"=>"20", "pdf"=>"2", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"0", "supp-data"=>"0", "cited-by"=>"0", "year"=>"2015", "month"=>"7"}
  • {"unique-ip"=>"24", "full-text"=>"25", "pdf"=>"5", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"0", "supp-data"=>"0", "cited-by"=>"0", "year"=>"2015", "month"=>"8"}
  • {"unique-ip"=>"37", "full-text"=>"41", "pdf"=>"3", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"15", "supp-data"=>"3", "cited-by"=>"0", "year"=>"2015", "month"=>"9"}
  • {"unique-ip"=>"30", "full-text"=>"41", "pdf"=>"6", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"13", "supp-data"=>"0", "cited-by"=>"0", "year"=>"2015", "month"=>"10"}
  • {"unique-ip"=>"60", "full-text"=>"57", "pdf"=>"6", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"36", "supp-data"=>"3", "cited-by"=>"0", "year"=>"2016", "month"=>"2"}
  • {"unique-ip"=>"32", "full-text"=>"41", "pdf"=>"7", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"15", "supp-data"=>"3", "cited-by"=>"0", "year"=>"2015", "month"=>"11"}
  • {"unique-ip"=>"23", "full-text"=>"23", "pdf"=>"3", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"5", "supp-data"=>"0", "cited-by"=>"0", "year"=>"2015", "month"=>"12"}
  • {"unique-ip"=>"40", "full-text"=>"49", "pdf"=>"5", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"13", "supp-data"=>"1", "cited-by"=>"0", "year"=>"2016", "month"=>"1"}
  • {"unique-ip"=>"61", "full-text"=>"83", "pdf"=>"1", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"19", "supp-data"=>"3", "cited-by"=>"0", "year"=>"2016", "month"=>"3"}
  • {"unique-ip"=>"72", "full-text"=>"97", "pdf"=>"4", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"29", "supp-data"=>"1", "cited-by"=>"0", "year"=>"2016", "month"=>"4"}
  • {"unique-ip"=>"90", "full-text"=>"124", "pdf"=>"0", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"71", "supp-data"=>"7", "cited-by"=>"0", "year"=>"2016", "month"=>"5"}
  • {"unique-ip"=>"72", "full-text"=>"95", "pdf"=>"5", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"42", "supp-data"=>"2", "cited-by"=>"0", "year"=>"2016", "month"=>"6"}
  • {"unique-ip"=>"93", "full-text"=>"108", "pdf"=>"9", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"23", "supp-data"=>"4", "cited-by"=>"0", "year"=>"2016", "month"=>"7"}
  • {"unique-ip"=>"104", "full-text"=>"88", "pdf"=>"51", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"22", "supp-data"=>"3", "cited-by"=>"0", "year"=>"2016", "month"=>"8"}
  • {"unique-ip"=>"141", "full-text"=>"160", "pdf"=>"29", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"33", "supp-data"=>"1", "cited-by"=>"0", "year"=>"2016", "month"=>"9"}
  • {"unique-ip"=>"384", "full-text"=>"412", "pdf"=>"99", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"79", "supp-data"=>"5", "cited-by"=>"0", "year"=>"2016", "month"=>"10"}
  • {"unique-ip"=>"131", "full-text"=>"150", "pdf"=>"3", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"40", "supp-data"=>"0", "cited-by"=>"0", "year"=>"2016", "month"=>"11"}
  • {"unique-ip"=>"206", "full-text"=>"260", "pdf"=>"2", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"31", "supp-data"=>"7", "cited-by"=>"0", "year"=>"2016", "month"=>"12"}
  • {"unique-ip"=>"196", "full-text"=>"244", "pdf"=>"15", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"60", "supp-data"=>"4", "cited-by"=>"0", "year"=>"2017", "month"=>"1"}
  • {"unique-ip"=>"397", "full-text"=>"468", "pdf"=>"3", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"63", "supp-data"=>"12", "cited-by"=>"0", "year"=>"2017", "month"=>"2"}
  • {"unique-ip"=>"672", "full-text"=>"780", "pdf"=>"7", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"110", "supp-data"=>"20", "cited-by"=>"0", "year"=>"2017", "month"=>"3"}
  • {"unique-ip"=>"561", "full-text"=>"697", "pdf"=>"1", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"69", "supp-data"=>"7", "cited-by"=>"0", "year"=>"2017", "month"=>"4"}
  • {"unique-ip"=>"264", "full-text"=>"379", "pdf"=>"8", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"86", "supp-data"=>"12", "cited-by"=>"0", "year"=>"2017", "month"=>"5"}
  • {"unique-ip"=>"732", "full-text"=>"860", "pdf"=>"55", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"74", "supp-data"=>"8", "cited-by"=>"0", "year"=>"2017", "month"=>"6"}
  • {"unique-ip"=>"195", "full-text"=>"227", "pdf"=>"100", "abstract"=>"0", "scanned-summary"=>"0", "scanned-page-browse"=>"0", "figure"=>"28", "supp-data"=>"4", "cited-by"=>"0", "year"=>"2017", "month"=>"7"}

Relative Metric

{"start_date"=>"2015-01-01T00:00:00Z", "end_date"=>"2015-12-31T00:00:00Z", "subject_areas"=>[]}
Loading … Spinner
There are currently no alerts