Under equilibrium conditions a negative CO2 pulse, i.e., artificial extraction and storage of some CO2 amount, decays at about the same rate as a positive pulse (Fig. 4A).
Under equilibrium conditions a negative CO2 pulse, i.e., artificial extraction and storage of some CO2 amount, decays at about the same rate as a positive pulse (Fig. 4A).
Not exact matches
In a new dissipative structure (either a steady state or a limit cycle), concentrations of chemicals and rates of mass - transfer between the system and surroundings will not be those characteristic of the previous
equilibrium state (or the nonequilibrium steady state that corresponds to it
under conditions of instability) but rather they will be the (perhaps quite different) average values which pertain to the new structure.
Under physiological
conditions, the tyrosine kinase Abl is found in two different spatial structures — an open and a closed state — which exist in a delicate
equilibrium.
Under various
conditions, the
equilibrium solubility can be exceeded to give a so - called supersaturated solution, which is metastable.
These cells can be isolated based on the expression of an amplified Hex Venus transgene and SSEA - 1 (V+S +) and exist
under ES cell
conditions in a steady - state
equilibrium with at least one other more ICM - like cell state, V − S +.
Manipulation of either FGF signalling or Nanog expression levels can alter the ratio of cell types present in this state and single Venus positive or negative cells can regenerate this
equilibrium with apparently identical kinetics
under self - renewing
conditions.
«Capital Asset Prices: A Theory of Market
Equilibrium under Conditions of Risk.»
Consider a box willed with gas,
under two
conditions: (1) the first box is in
equilibrium, at high temperature, and thus has a high energy content; (2) the second box has low energy content, but is out of
equilibrium: it is stirred by turbulent convection, produced by heating from below and cooling from above.
The section where Gibbs discusses this problem is titled, «The
Conditions of
Equilibrium for Heterogeneous Masses
under the Influence of Gravity,» with the most relevant discussion given on pages 144 and 145.
See the top post, which derives the actual state of an ideal gas atmosphere in both hydrostatic -LRB--RRB-
equilibrium and simultaneously in (iso) thermal
equilibrium, repeatedly demonstrated to be the state where the gas has maximum entropy and the state the ideal gas will go to
under the precise
conditions described by Jelbring.
«The Earth's climate system is highly nonlinear: inputs and outputs are not proportional, change is often episodic and abrupt, rather than slow and gradual, and multiple
equilibria are the norm... there is a relatively poor understanding of the different types of nonlinearities, how they manifest
under various
conditions, and whether they reflect a climate system driven by astronomical forcings, by internal feedbacks, or by a combination of both... [We] suggest a robust alternative to prediction that is based on using integrated assessments within the framework of vulnerability studies... It is imperative that the Earth's climate system research community embraces this nonlinear paradigm if we are to move forward in the assessment of the human influence on climate.»
Kirchhoff showed this radiative exchange must be equal
under the restrictive
condition of thermal
equilibrium.