Gyration and business gyration — they need more capacity than they had a month ago and at a point where meetings are sapping every ounce of energy and time that needs to be remixed.
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With each gyration, there's more room to pour gratitude into each curve.
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Seriously, there's enough frosted lighting, gyration, and awkwardly staged bedroom activity to rival The Room. Yeh-yeh-yeh.
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Since taking office, Trump has kept Washington hopping, with his adversaries never knowing what wild gyration will rock the capital next.
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It voted for Mr. Obama by a 28 percentage point margin in 230 and for Mr. Trump by 10 — a 228-point gyration.
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The gyration made its way from his arms to his shoulders to his hips, and soon he was doing a salsa-style dance.
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And I think what I've seen is executives and team leaders need more time in their day right now to take care of the emotional gyration market.
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Huber then couples these metrics with a long-term holding period to ensure he is not washed out of a position because of an emotional market gyration.
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Bobby Lee, CEO of Chinese bitcoin exchange BTCC, told CNBC the gyration in prices was normal as the true value for these assets have yet to be discovered.
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The uncertainty has caused some gyration in Honeywell's stock year to date, but thanks in part to Intelligrated's fast-growing business, Honeywell's quarterly results have been steadily improving.
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"Markets are reacting to every gyration in these sort of tweets and trade comments," Mitul Kotecha, senior emerging markets strategist at TD Securities, told CNBC's "Squawk Box" on Tuesday.
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We staked a claim in front with the beach walkers, body surfers and a doughy man with a Hula-Hoop, his appendage swinging in sync with each hip gyration.
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At the Bowery show, mixed into her bouncy, gyration-heavy, platinum blond hair–whipping set, Kiyoko gives several short, warm-and-fuzzy speeches about how lucky she feels to be here.
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"There are tentative signs that consumption of durable goods are slowing, suggesting that the gyration in asset markets and gradually rising mortgage payments might be starting to bite," Lam said in a report.
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He also constantly gestures for more throttle, which I hit on sheer faith alone, as I'm not sure even the car's sporty suspension and all-wheel drive will carry it around another screeching gyration.
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The immediate effects of the vote on the rest of the world — a sell-off in global stock markets and gyration in currency markets — have been painful and worrisome, but so far not out of control.
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The Joanne singer recently stopped by Radio Disney to answer a handful of important questions about herself, such as her favorite dance move (a hip gyration with lots of finger guns and head bobbing) and her all-time favorite Super Bowl performance, Michael Jackson, naturally.
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"It is almost a function of the fact that last month was so dull, then you get the disappointing ISM number and everyone kind of freaks out real fast and that is what has led to this two-day, very quick gyration lower as we were kind of lulled almost to sleep by the lack of volatility in September," said Detrick.
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Traders were uncertain what caused the sudden gyration in the currency on Friday, but some attributed the move to reports of French President François Hollande urging the European Union to take a tough line on negotiations with the U.K. as it prepared to formally begin the exit process from the EU. "Investors may have thought that negotiations are going to be easy, but today's flash crash has shown where the support [level for the pound] is and the reality is this that it won't be long before we may touch the low again," said Naeem Aslam, chief market analyst at ThinkMarkets, in a note.
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According to Eq.(11), when the light propagates along anisotropic directions, the gyration (or the electro-gyration) effects manifest themselves as oscillations of the azimuth of polarization ellipse occurring with changing phase retardation \boldsymbol\Gamma\, .
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In geometry, a gyration is a rotation in a discrete subgroup of symmetries of the Euclidean plane such that the subgroup does not also contain a reflection symmetry whose axis passes through the center of rotational symmetry. In the orbifold corresponding to the subgroup, a gyration corresponds to a rotation point that does not lie on a mirror, called a gyration point. For example, having a sphere rotating about any point that is not the center of the sphere, the sphere is gyrating. If it was rotating about its center, the rotation would be symmetrical and it would not be considered gyration.
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22(6), 1027-1031. . The electro-gyration effect induced by a powerful laser radiation (a so-called self-induced or dynamic electro-gyration) has been studied in the works Akhmanov S.A., Zhdanov B.V., Zheludev N.I., Kovrigin N.I., Kuznetsov V.I. (1979). "Nonlinear optical activity in crystals", Pis.ZhETF.
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The branching index measures the effect of long-chain branches on the size of a macromolecule in solution. It is defined as g = b2>/l2>, where sb is the mean square radius of gyration of the branched macromolecule in a given solvent, and sl is the mean square radius of gyration of an otherwise identical linear macromolecule in the same solvent at the same temperature. A value greater than 1 indicates an increased radius of gyration due to branching.
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Development of a motion-enabled controller began when development of the Wii console started in 2001. In that year, Nintendo licensed a number of motion-sensing patents from Gyration Inc., a company that produces wireless motion-sensing computer mice. Gyration had previously pitched their idea and patents of a motion controller to Sony and Microsoft, who both declined.
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Symmetries of a regular tridecagon. Vertices are colored by their symmetry positions. Blue mirrors are drawn through vertices and edge. Gyration orders are given in the center.
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Symmetries of a regular hendecagon. Vertices are colored by their symmetry positions. Blue mirror lines are drawn through vertices and edge. Gyration orders are given in the center.
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Symmetries of a regular heptadecagon. Vertices are colored by their symmetry positions. Blue mirror lines are drawn through vertices and edges. Gyration orders are given in the center.
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Symmetries of a regular enneadecagon. Vertices are colored by their symmetry positions. Blue mirror lines are drawn through vertices and edges. Gyration orders are given in the center.
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Symmetries of a regular pentagon. Vertices are colored by their symmetry positions. Blue mirror lines are drawn through vertices and edges. Gyration orders are given in the center.
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In magnetic spectroscopy (EPR, NMR), a microwave pulse (EPR) or a radio frequency pulse (NMR) in a strong ambient magnetic field is used as the energizing event. This turns the magnetic particles at an angle to the ambient field, resulting in gyration. The gyrating spins then induce a periodic current in a detector coil. Each spin exhibits a characteristic frequency of gyration (relative to the field strength) which reveals information about the analyte.
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Symmetries of a regular enneagon. Vertices are colored by their symmetry positions. Blue mirrors are drawn through vertices, and purple mirrors are drawn through edge. Gyration orders are given in the center.
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Radius of gyration or gyradius of a body about an axis of rotation is defined as the radial distance to a point which would have a moment of inertia the same as the body's actual distribution of mass, if the total mass of the body were concentrated. Mathematically the radius of gyration is the root mean square distance of the object's parts from either its center of mass or a given axis, depending on the relevant application. It is actually the perpendicular distance from point mass to the axis of rotation. One can represent a trajectory of a moving point as a body.
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Nintendo then commissioned Gyration to create a one-handed controller for it, which eventually became the "Gyropod", a more traditional gamepad which allowed its right half to break away for motion-control. At this point, Gyration brought in a separate design firm, Bridge Design, to help pitch its concept to Nintendo. Under requirement to "roughly preserve the existing Game Cube button layout", it experimented with different forms "through sketches, models and interviewing various hardcore gamers". By "late 2004, early 2005", however, Nintendo had come up with the Wii Remote's less traditional "wand shape", and the design of the Nunchuk attachment.
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The statistics of a single polymer chain depends upon the solubility of the polymer in the solvent. For a solvent in which the polymer is very soluble (a "good" solvent), the chain is more expanded, while for a solvent in which the polymer is insoluble or barely soluble (a "bad" solvent), the chain segments stay close to each other. In the limit of a very bad solvent the polymer chain merely collapses to form a hard sphere, while in a good solvent the chain swells in order to maximize the number of polymer-fluid contacts. For this case the radius of gyration is approximated using Flory's mean field approach which yields a scaling for the radius of gyration of: ::R_g \sim N^ u, where R_g is the radius of gyration of the polymer, N is the number of bond segments (equal to the degree of polymerization) of the chain and u is the Flory exponent.
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A winding of N turns is modeled by a gyrator with a gyration resistance of N ohms. Transducers that are not based on magnetic induction may not be represented by a gyrator. For instance, a Hall effect sensor is modelled by a transformer.
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GPC separates based on the size or hydrodynamic volume (radius of gyration) of the analytes. This differs from other separation techniques which depend upon chemical or physical interactions to separate analytes.Skoog, D.A. Principles of Instrumental Analysis, 6th ed.; Thompson Brooks/Cole: Belmont, California, 2006, Chapter 28.
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29, 294-298. . Zheludev N.I., Karasev V.Yu., Kostov Z.M. Nunuparov M.S.(1986) "Giant exciton resonance in nonlinear optical activity", Pis.ZhETF, 43(12), 578-581. The influence of electro-gyration on the photorefraction storage has been investigated in, Kukhtarev N.V., Dovgalenko G.E. (1986) "Self-diffraction electrogyration and electroellipticity in centrosymmetric crystals", Sov.
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Around the band gap, the Faraday effect shows resonance behavior. More generally, (ferromagnetic) semiconductors return both electro-gyration and a Faraday response in the high frequency domain. The combination of the two is described by gyroelectromagnetic media, for which gyroelectricity and gyromagnetism (Faraday effect) may occur at the same time.
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A path of this walk of N steps in three dimensions represents a conformation of a polymer with excluded volume interaction. Because of the self-avoiding nature of this model, the number of possible conformations is significantly reduced. The radius of gyration is generally larger than that of the ideal chain.
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Due to its extensive use as a cloning vector in research and industry, pUC19 is frequently used in research as a model plasmid. For example, biophysical studies on its naturally supercoiled state have determined its radius of gyration to be 65.6 nm and its Stokes radius to be 43.6 nm.
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Each winding is modeled by a gyrator. The gyration resistance of each gyrator is equal to the number of turns on the associated winding. Each permeance element is modeled by a capacitor. The value of each capacitor in farads is the same as the inductance of the associated permeance in henrys.
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In 1775, Arnold took out a patentG.B. Patent No.1113 30 December 1775. for a new form of compensation balance with a bimetallic spiral at the centre. This spiral actuated two weighted arms, making them move in and out from the centre, changing the radius of gyration, and thus the period of oscillation.
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Symmetries of a regular heptagon. Vertices are colored by their symmetry positions. Blue mirror lines are drawn through vertices and edges. Gyration orders are given in the center.John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp.
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This gyration continually displaces the tube with a component along the direction of the centripetal force acting on the projectile, so that work is continually done on the projectile as it advances through the machine. The centripetal force experienced by the projectile is the accelerating force, and is proportional to the projectile mass.
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Then radius of gyration can be used to characterize the typical distance travelled by this point. Suppose a body consists of n particles each of mass m. Let r_1, r_2, r_3, \dots , r_n be their perpendicular distances from the axis of rotation. Then, the moment of inertia I of the body about the axis of rotation is :I = m_1 r_1^2 + m_2 r_2^2 + \cdots + m_n r_n^2 If all the masses are the same (m), then the moment of inertia is I=m(r_1^2+r_2^2+\cdots+r_n^2). Since m = M/n (M being the total mass of the body), :I=M(r_1^2+r_2^2+\cdots+r_n^2)/n From the above equations, we have :MR_g^2=M(r_1^2+r_2^2+\cdots+r_n^2)/n Radius of gyration is the root mean square distance of particles from axis formula :R_g^2=(r_1^2+r_2^2+\cdots+r_n^2)/n Therefore, the radius of gyration of a body about a given axis may also be defined as the root mean square distance of the various particles of the body from the axis of rotation.
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The electrogyration effect can be easy explained on the basis of Curie and Neumann symmetry principles. In the crystals that exhibit centre of symmetry, natural gyration can not exist, since, due to the Neumann principle, the point symmetry group of the medium should be a subgroup of the symmetry group that describes the phenomena, which are properties of this medium. As a result, the gyration tensor possessing a symmetry of second-rank axial tensor - \infty 2\, is not a subgroup of centrosymmetric media and so the natural optical activity cannot exist in such media. According to the Curie symmetry principle, external actions reduce the symmetry group of the medium down to the group defined by intersection of the symmetry groups of the action and the medium.
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Disruption of occludin regulation is an important aspect of a number of diseases. Strategies to prevent and/or reverse occludin downregulation may be an important therapeutic target. Mutation of occludin are thought to be a cause of band-like calcification with simple gyration and polymicrogyria (BLC-PMG). BLC-PMG is an autosomal recessive neurologic disorder.
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This makes experimental determination of important quantities such as the root mean square end-to-end distance or the radius of gyration much simpler. Additionally, the theta condition is also satisfied in the bulk amorphous polymer phase. Thus, the conformations adopted by polymers dissolved in theta solvents are identical to those adopted in bulk polymer polymerization .
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The nanoparticles must be smaller than the radius of gyration of the polymer, in the case of PMMA this is about 6 nm. Additionally, as nanoparticles increase in size viscosity increases, slowing the process. For a pure polymer deposition speeds of 200 μm/s are achievable. Adding nanoparticles reduces speeds to 2 μm/s, but is still faster than regular Dip Pen Lithography.
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Symmetries of a regular decagon. Vertices are colored by their symmetry positions. Blue mirrors are drawn through vertices, and purple mirrors are drawn through edges. Gyration orders are given in the center. The regular decagon has Dih10 symmetry, order 20. There are 3 subgroup dihedral symmetries: Dih5, Dih2, and Dih1, and 4 cyclic group symmetries: Z10, Z5, Z2, and Z1.
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Symmetries of a regular tetradecagon. Vertices are colored by their symmetry positions. Blue mirrors are drawn through vertices, and purple mirrors are drawn through edge. Gyration orders are given in the center. The regular tetradecagon has Dih14 symmetry, order 28. There are 3 subgroup dihedral symmetries: Dih7, Dih2, and Dih1, and 4 cyclic group symmetries: Z14, Z7, Z2, and Z1.
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Microlissencephaly can be diagnosed by prenatal MRI. MRI is better than ultrasound when it comes to detecting microlissencephaly or MSGP prenatally. The ideal time for proper prenatal diagnosis is between the 34th and 35th gestational week which is the time when the secondary gyration normally terminates. In microlissencephaly cases, the primary sulci would be unusually wide and flat while secondary sulci would be missing.
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It was intended that France would procure the Lynx for its Navy and a heavily modified armed reconnaissance variant for the French Army,"A Gyration of WG.13s." Flight International, 15 August 1968. pp. 262-263. with the United Kingdom in return buying Aérospatiale Gazelle and Puma for its armed forces. In October 1969, the French Army cancelled its requirement for the Lynx,James 1991, p. 401.
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Intrinsically unfolded proteins, once purified, can be identified by various experimental methods. The primary method to obtain information on disordered regions of a protein is NMR spectroscopy. The lack of electron density in X-ray crystallographic studies may also be a sign of disorder. Folded proteins have a high density (partial specific volume of 0.72-0.74 mL/g) and commensurately small radius of gyration.
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Symmetries of a regular icosagon. Vertices are colored by their symmetry positions. Blue mirrors are drawn through vertices, and purple mirrors are drawn through edge. Gyration orders are given in the center. The regular icosagon has Dih20 symmetry, order 40. There are 5 subgroup dihedral symmetries: (Dih10, Dih5), and (Dih4, Dih2, and Dih1), and 6 cyclic group symmetries: (Z20, Z10, Z5), and (Z4, Z2, Z1).
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The muon, like its lighter sibling the electron, acts like a spinning magnet. The parameter known as the "g-factor" indicates how strong the magnet is and the rate of its gyration. The value of g is slightly larger than 2, hence the name of the experiment. This difference from 2 (the "anomalous" part) is caused by higher-order contributions from quantum field theory.
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Only when threatened with deposition was Richard forced to give in and let de la Pole go.Saul (1997), p. 158. A commission was set up to review and control royal finances for a year.Harriss (2005), p. 459. Richard was deeply perturbed by this affront to his royal prerogative, and from February to November 1387 went on a "gyration" (tour) of the country to muster support for his cause.
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Mobile studs are permitted. 4 Split or fitted indexes are allowed with a holding system except in extra-thin calibers where the holding system is not required. 5 Regulating systems with balance with radius of variable gyration are allowed insofar as they meet the conditions of article 3, subparagraph 1. ;Wheels 6 The wheels of the going train must be chamfered above and below and have a polished sink.
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Symmetries of a regular icositetragon. Vertices are colored by their symmetry positions. Blue mirrors are drawn through vertices, and purple mirrors are drawn through edge. Gyration orders are given in the center. The regular icositetragon has Dih24 symmetry, order 48. There are 7 subgroup dihedral symmetries: (Dih12, Dih6, Dih3), and (Dih8, Dih4, Dih2 Dih1), and 8 cyclic group symmetries: (Z24, Z12, Z6, Z3), and (Z8, Z4, Z2, Z1).
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The pervaded volume V scales as the cube of the chain size V \approx R^3 R is some length scale describing the chain conformation such as the radius of gyration or root-mean-square end-to-end distance of the chain. Typically the pervaded volume is very large relative to the space actually occupied by the chain as most of the pervaded volume is usually filled with solvent or other chains.
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In August 2000 they released their first single, "Super Gyration!," on 7 inch vinyl only. In July 2002, after featuring several times on John Peel's programme on the UK's BBC Radio 1 and being hailed as "the future of rock" by the British music press, the band signed with the V2 record label. Their self-titled debut album made a strong impression in the UK, as well as in Australia and New Zealand.
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In its coil state, the radius of gyration of the macromolecule scales as its chain length to the three-fifths power. As it passes through the coil–globule transition, it shifts to scaling as chain length to the half power (at the transition) and finally to the one third power in the collapsed state. The direction of the transition is often specified by the constructions 'coil-to- globule' or 'globule-to-coil' transition.
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Section modulus is a geometric property for a given cross-section used in the design of beams or flexural members. Other geometric properties used in design include area for tension and shear, radius of gyration for compression, and moment of inertia and polar moment of inertia for stiffness. Any relationship between these properties is highly dependent on the shape in question. Equations for the section moduli of common shapes are given below.
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The resulting clusters are irregular, but statistically self-similar. They are examples of mass fractals, whereby their mass M grows with their typical size characterized by the radius of gyration Rg as a power-law : M \propto R_g^d where d is the mass fractal dimension. Depending whether the aggregation is fast or slow, one refers to diffusion limited cluster aggregation (DLCA) or reaction limited cluster aggregation (RLCA). The clusters have different characteristics in each regime.
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The change in the small-angle scattering signatures when the interactions between polymers are tuned. From left to right there is an increase in the amount of Magnesium in the solution, which alleviates the coulomb repulsion (thus reducing the order). The main purpose of such scattering experiments involving polymers is to study unique properties of the sample of interest: # Determine the polymers "size" - radius of gyration. # Evaluating the structural and thermo-statistical behavior of a polymer, i.e.
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275-278) The full symmetry of the regular form is r192 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders. Each subgroup symmetry allows one or more degrees of freedom for irregular forms.
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GAFolder makes torsion angles moves within the ranges defined by the values and uncertainties of torsion angles predicted by PREDITOR. GAFolder evaluates protein models by the scoring function described below. Scoring function: Scoring function of GAFolder consists of knowledge based scores and chemical shift scores. The knowledge-based scores include: # radius of gyration score, # hydrogen bond energy, # number of hydrogen bonds, # bad contacts score, # disulfide bond score, # modified threading energy based on the Bryant and Lawrence potential.
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Jon Bross joined Up, an 8-man rhythm and funk group in Milwaukee, as a student at the University of Wisconsin-Whitewater (1989–1993) and later joined Gyration (a 10-man disco and funk review) on rhythm guitar. David Jeffrey," Three Colorado Springs arts and business leaders recognized at lunch". The Gazette. By Jen Mulson born and raised in Alexandria, Alabama, played music in church and studied at Jacksonville (Alabama) State University and The Atlanta Institute of Music.
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He redesigned the compensation balance and developed two designs that showed promise. Known as the "T" and "S" balances, and marked as such in Arnold's 1782 patent (probably because of their appearance), both employed bimetallic strips of brass and steel with weights attached, which changed the radius of gyration with change in temperature. Although these probably needed a lot of adjustment, they appear to have worked well compared to his previous attempts at a compensation balance.
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Bursian was one of the pioneers of Soviet physics who played a large role in the development of theoretical physics in the USSR. Bursian carried out studies on the physics of currents in gases and vacuum, on Dispersion (optics) and gyration, the electronic theory of matter and the kinetics of chain reactions. He was the first to develop electrophysical methods in geological exploration. Bursian is the author of a number of scientific works on theoretical physics.
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The space occupied by a polymer molecule is generally expressed in terms of radius of gyration, which is an average distance from the center of mass of the chain to the chain itself. Alternatively, it may be expressed in terms of pervaded volume, which is the volume spanned by the polymer chain and scales with the cube of the radius of gyration.Rubinstein, p. 13 The simplest theoretical models for polymers in the molten, amorphous state are ideal chains.
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"Airliner Crashes After Explosion" The Argus – 1 February 1945, p.3 (National Library of Australia) Retrieved 25 May 2012 The main wreckage consisting of the fuselage, right inner wing, and left inner wing still with its engine attached, struck the ground inverted and was immediately consumed by fire. The bodies of the eight passengers were found in what remained of the cabin but were burned beyond recognition. The violent gyration of the fuselage threw the two pilots through the roof of the cockpit.
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There is, however, a one-time displacement in the direction of the force equal to (f/m)ωc−2, which should be considered a consequence of the polarization drift (see below) while the force is being turned on. The resulting motion is a cycloid. More generally, the superposition of a gyration and a uniform perpendicular drift is a trochoid. All drifts may be considered special cases of the force drift, although this is not always the most useful way to think about them.
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The dance involves a rotating movement of the neck ("wine" refers to winding, or gyration.) The dancer can also move their legs like a bird, while simultaneously rotating their wrists, neck, and posterior. Sometimes more advanced dancers will include splits in their Dutty Wine. The dance experienced a surge of popularity around the world, especially in communities in parts of the United Kingdom and North America. Some even have gone so far as to label it as "the dance craze" of 2006.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) The full symmetry of the regular form is r52 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries n are labeled as g for their central gyration orders.
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PCR product compared to a DNA ladder. In the case of nucleic acids, the direction of migration, from negative to positive electrodes, is due to the naturally occurring negative charge carried by their sugar-phosphate backbone. Double-stranded DNA fragments naturally behave as long rods, so their migration through the gel is relative to their size or, for cyclic fragments, their radius of gyration. Circular DNA such as plasmids, however, may show multiple bands, the speed of migration may depend on whether it is relaxed or supercoiled.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) The full symmetry of the regular form is r44 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries n are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) Full symmetry of the regular form is r18 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) Full symmetry of the regular form is r22 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) Full symmetry of the regular form is r40 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) Full symmetry of the regular form is r20 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275–278) Full symmetry of the regular form is r34 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) Full symmetry of the regular form is r38 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275–278) Full symmetry of the regular form is r26 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) Full symmetry of the regular form is r28 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) The full symmetry of the regular form is labeled r68 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries n are labeled as g for their central gyration orders.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) Full symmetry of the regular form is r10 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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He has recently made important advances in studying the water balance over global ocean and their influence on terrestrial and cryospheric water cycles, using a combination of space-based observations. Through 17 years as Team Leader and 14 years as Project Scientist, Timothy Liu was able to lead various groups of scientists through many cycles of fiscal gyration and changes of national and institutional priority, securing their funding support, communicating and promoting their results to the science community and to the public, and keeping the team spirit and cohesiveness.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) The full symmetry of the regular form is r56 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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As a wing stalls, aileron effectiveness is reduced, making the plane hard to control and increasing the risk of a spin starting. Post stall, steady flight beyond the stalling angle (where the coefficient of lift is largest) requires engine thrust to replace lift as well as alternative controls to replace the loss of effectiveness of the ailerons. For high- powered aircraft, the loss of lift (and increase in drag) beyond the stall angle is less of a problem than maintaining control. Some aircraft may be subject to post-stall gyration (e.g.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) The full symmetry of the regular form is r96 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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The potential functions used in GeNMR are derived from those used in CS23D and Proteus2. The knowledge-based potentials include information on predicted/known secondary structure, radius of gyration, hydrogen bond energies, number of hydrogen bonds, allowed backbone and side chain torsion angles, atom contact radii (bump checks), disulfide bonding information and a modified threading energy based on the Bryant and Lawrence potential. The chemical shift component of the GeNMR potential uses weighted correlation coefficients calculated between the observed and SHIFTX calculated shifts of the structure being refined.
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John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, (2008) The Symmetries of Things, (Chapter 20, Generalized Schaefli symbols, Types of symmetry of a polygon pp. 275-278) The full symmetry of the regular form is r48 and no symmetry is labeled a1. The dihedral symmetries are divided depending on whether they pass through vertices (d for diagonal) or edges (p for perpendiculars), and i when reflection lines path through both edges and vertices. Cyclic symmetries in the middle column are labeled as g for their central gyration orders.
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Some of the most interesting characteristics exhibited by star- shaped polymers are their unique rheological and dynamic properties compared to linear analogues of identical molecular weight and monomer composition. Generally, they have smaller hydrodynamic radii, radii of gyration and lower internal viscosities than linear analogues of the same molecular weight. Internal viscosity increases with increased functionality and molecular weight of branches with the effects of functionality eventually saturating, leaving viscosity dependent only on molecular weight of the arms. Heteroarm stars have observed viscosities and hydrodynamic radii higher than homostars.
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Early diagnosis of the ZTTK syndrome can be determined by brain imaging. Magnetic resonance imaging (MRI) of the brain of ZTTK syndrome patients have revealed significant abnormalities. Abnormal gyration patterns were seen, including polymicrogyria; many unusually small folds in the brain, simplified gyria; reduced number and shallow appearance of gyri, and periventricular nodular heterotopia; failure of neurons to migrate properly during early development of the fetal brain. Ventriculomegaly can also be observed in MRI where the lateral ventricles become dilated in the foetus and can contribute to developmental delays in ZTTK syndrome individual.
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The USBC and World Bowling promulgate bowling ball specifications. USBC specifications include physical requirements for weight (≤), diameter (—), surface hardness, surface roughness, hole drilling limitations (example: a single balance hole including the thumb hole for "two-handed" bowlers), balance, plug limitations, and exterior markings (structural and commercial), as well as requirements for dynamic performance characteristics such as radius of gyration (RG; 2.46—2.80), RG differential (≤0.06), and coefficient of friction (≤0.32). The USBC banned weight holes (balance holes) in competition, effective August 1, 2020, to prevent their changing ball dynamics.
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In comparison to most single-engine aircraft, it possesses superior power loading and above average wing loading. The original model of the SF.260 was powered by a single Lycoming O-540 engine, capable of providing 260 hp. The standard model made use of a carburetor, while fully aerobatic models featured fuel injection instead. The SF.260 has been described as having the power to be immune to the gyration-like effects of turbulence and possessing a high rate of climb. During the 1980s, aerospace publication Flying Magazine stated the SF.260 to be: "the fastest normally aspirated piston single in production".
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Often called "air mice" since they do not require a surface to operate, inertial mice use a tuning fork or other accelerometer (US Patent 4787051) to detect rotary movement for every axis supported. The most common models (manufactured by Logitech and Gyration) work using 2 degrees of rotational freedom and are insensitive to spatial translation. The user requires only small wrist rotations to move the cursor, reducing user fatigue or "gorilla arm". Usually cordless, they often have a switch to deactivate the movement circuitry between use, allowing the user freedom of movement without affecting the cursor position.
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The Highcliff is one example of an extremely slender skyscraper. In architecture, the slenderness ratio, or simply slenderness is the quotient between the height and the width of a building. In structural engineering, slenderness is a measure of the propensity of a column to buckle. It is defined as l/k where l is the effective length of the column and k is the least radius of gyration, the latter defined by k^2=I/A where A is the area of the cross-section of the column and I is the second moment of area of the cross-section.
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With the video, scholars noted the expression of Venetian vitality in it. Author Margaret Plant (2002) commented: "With the lion of Saint Mark and the virginal city to the forefront, old sacrosanct Venice was propelled into a pop world of high-energy gyration, and endless circulation." She also noted that Saint Mark was a symbol of a time when sexual crime was punished severely in Venice and acts of rape, homosexuality and fornication incurred the loss of a nose, a hand or sometimes life itself. Madonna appeared to challenge such brutality and stretch the boundaries of tolerance in the video.
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The development of extensional rheometers has proceeded more slowly than shear rheometers, due to the challenges associated with generating a homogeneous extensional flow. Firstly, interactions of the test fluid or melt with solid interfaces will result in a component of shear flow, which will compromise the results. Secondly, the strain history of all the material elements must be controlled and known. Thirdly, the strain rates and strain levels must be high enough to stretch the polymeric chains beyond their normal radius of gyration, requiring instrumentation with a large range of deformation rates and a large travel distance.
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Jet damping or thrust damping is the effect of rocket exhaust removing energy from the transverse angular motion of a rocket. If a rocket has pitch or yaw motion then the exhaust must be accelerated laterally as it flows down the exhaust tube and nozzle. Once the exhaust leaves the nozzle this lateral momentum is lost to the vehicle and thus serves to damp the lateral oscillations. The jet damping is stabilizing as long as the distance from the instantaneous spacecraft center of mass to the nozzle exit plane exceeds the instantaneous transverse radius of gyration.
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The time scale and recurrence patterns of these orbital period modulations suggested to Matese and Whitmire (1983) a mechanism invoking changes in the quadrupole moment of one star with subsequent spin- orbit coupling. However, they could not provide any convincing explanation for what might cause such fluctuations in the quadrupole moment. Taking the Matese and Whitmire mechanism as a basis, Applegate argued that changes in the radius of gyration of one star could be related to magnetic activity cycles. Supportive evidence for his hypothesis came from the observation that a large fraction of the late-type secondary stars of Algol binaries appear to be rapidly rotating convective stars, implying that they should be chromospherically active.
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When polymers crystallize from an isotropic, bulk of melt or concentrated solution, the crystalline lamellae (10 to 20 nm in thickness) are typically organized into a spherulitic morphology as illustrated above. However, when polymer chains are confined in a space with dimensions of a few tens of nanometers, comparable to or smaller than the lamellar crystal thickness or the radius of gyration, nucleation and growth can be dramatically affected. As an example, when a polymer crystallizes in a confined ultrathin layer, the isotropic spherulitic organization of lamellar crystals is hampered and confinement can produce unique lamellar crystal orientations. Sometimes the chain alignment is parallel to the layer plane and the crystals are organized as ‘‘on-edge’’ lamellae.
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A higher differential indicates greater track flare potential—more angular motion from the break point to the pocket—and a lower differential indicates lower flare potential and a smoother arc to the hook. The lesser-used intermediate differential rating (sometimes termed mass bias rating) quantifies the degree to which a bowling ball core is symmetrical or asymmetrical. Analytically, ID is defined by the USBC as the "difference in radius of gyration between the Y (high RG) and Z (intermediate RG) axes". In practice, a higher ID indicates greater asymmetry, which causes more area to be created at the break point to cause the ball to respond more quickly to friction than symmetrical balls.
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The slenderness ratio of a wall is defined as a function of the effective height divided by either the effective thickness or the radius of the gyration of the wall section. It is highly related to the slenderness limit that is the cut-off between elements being classed "slender" or "stocky". Slender walls are vulnerable to buckling failure modes, including Euler in-plane buckling due to axial compression, Euler out-of-plane buckling due to axial compression and lateral torsional buckling due to bending moment. In the design process, structural engineers need to consider all these failure modes to ensure that the wall design is safe under various kinds of possible loading conditions.
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Ideal MHD is only strictly applicable when: # The plasma is strongly collisional, so that the time scale of collisions is shorter than the other characteristic times in the system, and the particle distributions are therefore close to Maxwellian. # The resistivity due to these collisions is small. In particular, the typical magnetic diffusion times over any scale length present in the system must be longer than any time scale of interest. # Interest in length scales much longer than the ion skin depth and Larmor radius perpendicular to the field, long enough along the field to ignore Landau damping, and time scales much longer than the ion gyration time (system is smooth and slowly evolving).
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The secondary component was identified as the radio emitting source in Algol using Very-long-baseline interferometry by Lestrade and co- authors. Magnetic activity cycles in the chromospherically active secondary component induce changes in its radius of gyration that have been linked to recurrent orbital period variations on the order of ≈ 10−5 via the Applegate mechanism. Mass transfer between the components is small in the Algol system but could be a significant source of period change in other Algol-type binaries. Algol is about 92.8 light-years from the Sun, but about 7.3 million years ago it passed within 9.8 light-years of the Solar System and its apparent magnitude was about −2.5, which is considerably brighter than the star Sirius is today.
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If the Earth moves around the Sun, the necessary movements were the annual motion of the Earth, the diurnal motion of the Earth, and the rotation of the sun. However, if the Sun moved around the Earth, this accounted for the same movement as both the annual and diurnal motions in the Copernican model. In addition, the annual gyration of the Sun at its poles, and the rotation of the Sun had to be added to completely account for the movement of sunspots. While both models required three movements, the heliocentric model required the Earth to make two movements (annual and diurnal) which could not be demonstrated, while the geocentric model was based on three observable celestial movements, and was accordingly preferable.
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The random coil of E. coli chromosomal DNA would occupy a volume (4/3 π r3) of ~ 523 µm3, calculated from the radius of gyration (Rg = (√N a)/√6) where a is the Kuhn length (2 x persistence length), and N is the number of Kuhn length segments in the DNA (total length of the DNA divided by a). Although DNA is already condensed in the random coil form, it still cannot assume the volume of the nucleoid which is less than a micron. Thus, the inherent property of DNA is not sufficient: additional factors must help condense DNA further on the order of ~103 (volume of the random coil divided by the nucleoid volume). The second essential aspect of nucleoid formation is the functional arrangement of DNA.
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For a collection of objects revolving about a center, for instance all of the bodies of the Solar System, the orientations may be somewhat organized, as is the Solar System, with most of the bodies' axes lying close to the system's axis. Their orientations may also be completely random. In brief, the more mass and the farther it is from the center of rotation (the longer the moment arm), the greater the moment of inertia, and therefore the greater the angular momentum for a given angular velocity. In many cases the moment of inertia, and hence the angular momentum, can be simplified by, :I=k^2m, :where k is the radius of gyration, the distance from the axis at which the entire mass m may be considered as concentrated.
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Similarly, though manufacturer literature often describes specific core shapes, differently-shaped cores can make exactly the same contribution to ball motion if they have the same overall RG characteristics. "Weak" layouts ("pin down": pin between finger and thumb holes) hook sooner but have milder backend reaction, while "strong" layouts ("pin up": pin further from thumb hole than finger holes) enable greater skid lengths and more angular backend reaction. Manufacturers commonly cite specifications relating to a bowling ball's core, include radius of gyration (RG), differential of RG (commonly abbreviated differential), and intermediate differential (also called mass bias). Analytically, the United States Bowling Congress defines RG as "the distance from the axis of rotation at which the total mass of a body might be concentrated without changing its moment of inertia".
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Following his impeachment, de la Pole had had his royal grants of land reversed (although he retained his earldom), and was sentenced to be imprisoned, probably in Corfe Castle. The King soon overturned these judgments; not only was de la Pole soon set free, but he joined the King for the Christmas festivities at Windsor later that year, where Richard treated him with "ostentatious warmth." In New Year 1387, the King left London for a prolonged period (on what has been known as his "gyration" around the country), The word gyrare is used by the contemporary chronicler Henry Knighton, the at-least partial goal of which was to gather together and consolidate his supporters. Not only did Richard ignore the parliament-imposed council, but, whilst he was out of London, he even held councils of his own.
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A 2005-2008 USBC Ball Motion Study found that the ball design factors that most contributed to ball motion were the microscopic "spikes" and pores on the ball's surface (considered part of chemical frictional characteristics), the respective coefficients of friction between ball and lane in the oiled and dry parts of the lane, and the ball's oil absorption rate, followed in dominance by certain characteristics of the ball's core (mainly radius of gyration, and total differential). Freeman and Hatfield (2018) explain that in most circumstances it is chemical friction—controlled by the manufacturer's proprietary coverstock formulation governing its "stickiness"—that primarily determines ball motion. Further, surface finish—modifiable by sandpaper, polish and the like—is also a material factor. Though manufacturer literature often specifies track flare—exhibited by successive tracks of oil in a "bowtie" pattern and caused by RG differential—the USBC ball motion study showed flare's influence to be small, assuming that a minimal threshold of flare exists to present a "dry" surface for successive ball revolutions.
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The Hucklebuck became a wildly successful dance craze in 1949, partly due to its sexual connotations. LeRoi Jones reported that people danced at rent parties in Newark, night after night "until they dropped." The basic dance has been described as having "a double point with the feet to the side on each side (four counts) then a lift and twist of the leg and a small kick, then a shimmy, hip gyration... The dance could get very sexual in nature when done as a couple dance with the male dancing behind the female, one hand on her waist or hip and the other on her shoulder, gyrating the hips in unison or with shocking variations such as when the female dancers would lie down on their backs and the male dancers would stand over the center of her, slowly doing hip gyrations, hip rolling, wiggling dance movements, slowly working their way over and past the female's head." "The Hucklebuck Dance", StreetSwing.com. Retrieved 20 October 2015 The Hucklebuck was featured in one of the original 39 “The Honeymooners” episode 20, “Young at Heart” in 1956.
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