翻訳と辞書 Words near each other ・ Quaternion ・ Quaternion (disambiguation) ・ Quaternion (poetry) ・ Quaternion algebra ・ Quaternion group ・ Quaternion Society ・ Quaternion-Kähler manifold ・ Quaternion-Kähler symmetric space ・ Quaternionic analysis ・ Quaternionic discrete series representation ・ Quaternionic matrix ・ Quaternionic projective space ・ Quaternionic representation ・ Quaternionic structure ・ Quaternionic vector space ・ Quaternions and spatial rotation ・ Quaternium ・ Quaternium-15 ・ Quatford ・ Quathiaski Cove ・ Quathlambia ・ Quatiara luctuosa ・ Quatiguá ・ Quatinga Velho ・ Quatipuru ・ Quatis ・ Quatit, Eritrea ・ Quatlecoatl ・ Quatloo ・ Quatloos.com Dictionary Lists mini英和辞書 mini和英辞書 Webster 1913 Latin-English FOLDOC Wikipedia English ウィキペディア

翻訳と辞書　辞書検索 [ 開発暫定版 ] スポンサード リンク Quaternions and spatial rotation ： ウィキペディア英語版 Quaternions and spatial rotation Unit quaternions, also known as versors, provide a convenient mathematical notation for representing orientations and rotations of objects in three dimensions. Compared to Euler angles they are simpler to compose and avoid the problem of gimbal lock. Compared to rotation matrices they are more numerically stable and may be more efficient. Quaternions have found their way into applications in computer graphics, computer vision, robotics, navigation, molecular dynamics, flight dynamics,〔Amnon Katz (1996) ''Computational Rigid Vehicle Dynamics'', Krieger Publishing Co. ISBN 978-1575240169〕 orbital mechanics of satellites〔J. B. Kuipers (1999) ''Quaternions and rotation Sequences: a Primer with Applications to Orbits, Aerospace, and Virtual Reality'', Princeton University Press ISBN 978-0-691-10298-6〕 and crystallographic texture analysis. When used to represent rotation, unit quaternions are also called rotation quaternions. When used to represent an orientation (rotation relative to a reference coordinate system), they are called orientation quaternions or attitude quaternions. == Using quaternion rotations == In 3-dimensional space, according to Euler's rotation theorem, any rotation or sequence of rotations of a rigid body or coordinate system about a fixed point is equivalent to a single rotation by a given angle about a fixed axis (called ''Euler axis'') that runs through the fixed point. The Euler axis is typically represented by a unit vector . Therefore, any rotation in three dimensions can be represented as a combination of a vector  and a scalar . Quaternions give a simple way to encode this axis–angle representation in four numbers, and can be used to apply the corresponding rotation to a position vector, representing a point relative to the origin in R3. A Euclidean vector such as or can be rewritten as or , where , , are unit vectors representing the three Cartesian axes. A rotation through an angle of around the axis defined by a unit vector : $\backslash vec\; =\; (u\_x,\; u\_y,\; u\_z)\; =\; u\_x\backslash mathbf\; +\; u\_y\backslash mathbf\; +\; u\_z\backslash mathbf$ can be represented by a quaternion. This can be done using an extension of Euler's formula: : $\backslash mathbf\; =\; e^\; +\; u\_z\backslash mathbf)\}\}\; =\; \backslash cos\; \backslash frac\; +\; (u\_x\backslash mathbf\; +\; u\_y\backslash mathbf\; +\; u\_z\backslash mathbf)\; \backslash sin\; \backslash frac$ It can be shown that the desired rotation can be applied to an ordinary vector $\backslash mathbf\; =\; (p\_x,\; p\_y,\; p\_z)\; =\; p\_x\backslash mathbf\; +\; p\_y\backslash mathbf\; +\; p\_z\backslash mathbf$ in 3-dimensional space, considered as a quaternion with a real coordinate equal to zero, by evaluating the conjugation of  by : : $\backslash mathbf\; =\; \backslash mathbf\; \backslash mathbf\; \backslash mathbf^$ using the Hamilton product, where is the new position vector of the point after the rotation. In a programmatic implementation, this is achieved by constructing a quaternion whose vector part is p and real part equals zero and then performing the quaternion multiplication. The vector part of the resulting quaternion is the desired vector p'. Mathematically, this operation carries the ''set'' of all "pure" quaternions p (those with real part equal to zero) — which constitute a 3-dimensional space among the quaternions — into itself, by the desired rotation about the axis ''u'', by the angle θ. (Each real quaternion is carried into itself by this operation. But for the purpose of rotations in 3-dimensional space, we ignore the real quaternions.) The rotation is clockwise if our line of sight points in the same direction as . In this instance, is a unit quaternion and : $\backslash mathbf^\; =\; e^\; +\; u\_z\backslash mathbf)\}\}\; =\; \backslash cos\; \backslash frac\; -\; (u\_x\backslash mathbf\; +\; u\_y\backslash mathbf\; +\; u\_z\backslash mathbf)\; \backslash sin\; \backslash frac\; .$ It follows that conjugation by the product of two quaternions is the composition of conjugations by these quaternions: If and are unit quaternions, then rotation (conjugation) by  is :$\backslash mathbf\; \backslash vec\; (\backslash mathbf)^\; =\; \backslash mathbf\; \backslash vec\; \backslash mathbf^\; \backslash mathbf^\; =\; \backslash mathbf\; (\backslash mathbf\; \backslash vec\; \backslash mathbf^)\; \backslash mathbf^$, which is the same as rotating (conjugating) by  and then by . The scalar component of the result is necessarily zero. The quaternion inverse of a rotation is the opposite rotation, since $\backslash mathbf^\; (\backslash mathbf\; \backslash vec\; \backslash mathbf^)\; \backslash mathbf\; =\; \backslash vec$. The square of a quaternion rotation is a rotation by twice the angle around the same axis. More generally is a rotation by  times the angle around the same axis as . This can be extended to arbitrary real , allowing for smooth interpolation between spatial orientations; see Slerp. Two rotation quaternions can be combined into one equivalent quaternion by the relation: : $\backslash mathbf\text{'}\; =\; \backslash mathbf\_2\; \backslash mathbf\_1$ in which corresponds to the rotation followed by the rotation . (Note that quaternion multiplication is not commutative.) Thus, an arbitrary number of rotations can be composed together and then applied as a single rotation. 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Quaternions and spatial rotation」の詳細全文を読む スポンサード リンク 翻訳と辞書 : 翻訳のためのインターネットリソース Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.