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  2. LibreOffice - Wikipedia

    en.wikipedia.org/wiki/LibreOffice

    LibreOffice (/ ˈ l iː b r ə /) [11] is a free and open-source office productivity software suite, a project of The Document Foundation (TDF). It was forked in 2010 from OpenOffice.org , an open-sourced version of the earlier StarOffice .

  3. Scribus - Wikipedia

    en.wikipedia.org/wiki/Scribus

    Scribus 1.5.7 improves undo and redo action. Qt 5.14 is new base for compilation and 3rd party components have newer versions. Next version is 1.5.8 as perhaps last step before 1.6.0. [22] From view of developers Version 1.5.7 is stable. There are no new Versions in pipe with Backports for the 1.4 tree with the near end of QT4 support in most ...

  4. Harley Quinn - Wikipedia

    en.wikipedia.org/wiki/Harley_Quinn

    Harley Quinn (Dr. Harleen Frances Quinzel, PhD) is a fictional character appearing in American comic books published by DC Comics.She was created by Paul Dini and Bruce Timm for Batman: The Animated Series as a henchwoman for the Joker, and debuted in its 22nd episode, "Joker's Favor", on September 11, 1992.

  5. Don Quixote - Wikipedia

    en.wikipedia.org/wiki/Don_Quixote

    For Cervantes and the readers of his day, Don Quixote was a one-volume book published in 1605, divided internally into four parts, not the first part of a two-part set. The mention in the 1605 book of further adventures yet to be told was totally conventional, did not indicate any authorial plans for a continuation, and was not taken seriously by the book's first readers.

  6. Android version history - Wikipedia

    en.wikipedia.org/wiki/Android_version_history

    The version history of the Android mobile operating system began with the public release of its first beta on November 5, 2007. The first commercial version, Android 1.0, was released on September 23, 2008. The operating system has been developed by Google on a yearly schedule since at least 2011. [1]

  7. Maxwell's equations - Wikipedia

    en.wikipedia.org/wiki/Maxwell's_equations

    The integral version of Gauss's equation can thus be rewritten as = Since Ω is arbitrary (e.g. an arbitrary small ball with arbitrary center), this is satisfied if and only if the integrand is zero everywhere. This is the differential equations formulation of Gauss equation up to a trivial rearrangement.

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