We also need to recognize that in many places, being a nonconservative can be hard.
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"You have people who are socially conservative and fiscally nonconservative and vice versa," Trump told me.
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The result was that the debates and calendar helped nominate the most nonconservative candidate in ages: Donald J. Trump.
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They have been trained for generations, stretching back to the 1950s, to view news media as inherently ideological, and to reject nonconservative sources.
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Her alliance with the Dixie Chicks, country pariahs for so long for their outspoken, nonconservative politics, on the stage of country music's most prestigious awards show, was a robust victory for tolerance.
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Some focus on electing a centrist, independent presidential candidate; a quixotic and indeed foolish idea, since such a candidate could never win 270 electoral votes and would only split the nonconservative vote, ensuring Republican victory.
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Mr. Trump can reach out to independent voters in 2018 by more forcefully advocating nonconservative ideas, like the oft-teased infrastructure bill, which would spend taxpayer money on a host of projects in what would almost certainly be a foolhardy way.
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One of the first well-characterized mutants of EPX was a G→A transition resulting in a nonconservative mutation at the protein level.
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However, for any sufficiently detailed description, all these forces are the results of conservative ones since each of these macroscopic forces are the net results of the gradients of microscopic potentials. The connection between macroscopic nonconservative forces and microscopic conservative forces is described by detailed treatment with statistical mechanics. In macroscopic closed systems, nonconservative forces act to change the internal energies of the system, and are often associated with the transfer of heat. According to the Second law of thermodynamics, nonconservative forces necessarily result in energy transformations within closed systems from ordered to more random conditions as entropy increases.
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The most known empirical models in hysteresis are Preisach and Jiles-Atherton models. These models allow an accurate modeling of the hysteresis loop and are widely used in the industry. However, these models lose the connection with thermodynamics and the energy consistency is not ensured. A more recent model, with a more consistent thermodynamic foundation, is the vectorial incremental nonconservative consistent hysteresis (VINCH) model of Lavet et al. (2011).
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This way of mixing tracers is very important, giving a baseline of what value of a tracer one should expect. The value of a tracer as a point is expected to be an average value of the sources that flow into that region. Deviations from this are indicative of other processes. These can be called nonconservative mixing, where there are other processes that do not conserve the amount of tracer.
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For certain physical scenarios, it is impossible to model forces as being due to gradient of potentials. This is often due to macrophysical considerations that yield forces as arising from a macroscopic statistical average of microstates. For example, friction is caused by the gradients of numerous electrostatic potentials between the atoms, but manifests as a force model that is independent of any macroscale position vector. Nonconservative forces other than friction include other contact forces, tension, compression, and drag.
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By using his results, it is easy to prove that functions of bounded variation form an algebra of discontinuous functions: in particular, using his calculus for , it is possible to define the product of the Heaviside step function and the Dirac distribution in one variable.See . This paper is one of several works where the results of the paper are extended in order to define a particular product of distributions: the product introduced is called the "Nonconservative product".
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Fedora has its own beta cycle and has some issues fixed by contributors who include Red Hat staff. However, its quick and nonconservative release cycle means it might not be suitable for some users. Fedora is somewhat a test-bed for Red Hat, allowing them to beta test their new features before they get included in Red Hat Enterprise Linux. Since the release of Fedora, Red Hat has no longer made binary versions of its commercial product available free-of-charge.
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If only these two original criteria are used to define hypoelasticity, then hyperelasticity would be included as a special case, which prompts some constitutive modelers to append a third criterion that specifically requires a hypoelastic model to not be hyperelastic (i.e., hypoelasticity implies that stress is not derivable from an energy potential). If this third criterion is adopted, it follows that a hypoelastic material might admit nonconservative adiabatic loading paths that start and end with the same deformation gradient but do not start and end at the same internal energy. Note that the second criterion requires only that the function G exists.
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However, it has been argued that this model would actually generate 1/f2 noise rather than 1/f noise. This claim was based on untested scaling assumptions, and a more rigorous analysis showed that sandpile models generally produce 1/fa spectra, with a<2\. Other simulation models were proposed later that could produce true 1/f noise, and experimental sandpile models were observed to yield 1/f noise. In addition to the nonconservative theoretical model mentioned above, other theoretical models for SOC have been based upon information theory , mean field theory , the convergence of random variables , and cluster formation.
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From various genome analyses, it was concluded that the double-strand breaks (DSB) can be repaired via homologous recombination by at least two different but related pathways. In case of major pathway, homologous sequences on both sides of the DSB will be employed which seems to be analogous to the conservative DSB repair model that was originally proposed for meiotic recombination in yeast. where as the minor pathway is restricted to only one side of the DSB as postulated by nonconservative one-sided invasion model. However, in both cases the sequence of the recombination partners will be absolutely conserved.
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It is the macroscopic energy associated with a system. The principle of conservation of mechanical energy states that if an isolated system is subject only to conservative forces, then the mechanical energy is constant. If an object moves in the opposite direction of a conservative net force, the potential energy will increase; and if the speed (not the velocity) of the object changes, the kinetic energy of the object also changes. In all real systems, however, nonconservative forces, such as frictional forces, will be present, but if they are of negligible magnitude, the mechanical energy changes little and its conservation is a useful approximation.
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Garret Moddel at University of Colorado has highlighted that he believes such devices hinge on the assumption that the Casimir force is a nonconservative force, he argues that there is sufficient evidence (e.g. analysis by Scandurra (2001)) to say that the Casimir effect is a conservative force and therefore even though such an engine can exploit the Casimir force for useful work it cannot produce more output energy than has been input into the system. In 2008, DARPA solicited research proposals in the area of Casimir Effect Enhancement (CEE). The goal of the program is to develop new methods to control and manipulate attractive and repulsive forces at surfaces based on engineering of the Casimir force.
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