no.
Maximum entropy is when thermal equilibrium is reached and no further vaporisation is possible.
carbon dioxide and water :)
N2 +
Rest implies stationary, equilibrium implies a resultant force of zero. Therefore, a body in equilibrium could be moving, for example a sky diver at terminal velocity, where resistive forces are equal to the force of gravity. This means that a body can be in equilibrium and not at rest, but a body at rest MUST be in equilibrium, otherwise it would move. So, to answer the question is: It's impossible.
2
To be permeable to gases & impermeable to liquids. To be as large as possible.
Evaporation from a sealed impermeable container is not possible.
yess
The Smallest unit of an covalent bond is a molecule
2 structures are possible for a tetrahedral molecule with a formula of AHXYZ.
The equilibrium distribution of a molecule across a membrane depends on concentration and membrane potential. A charged molecule will respond to both components of the electrochemical gradient and will distribute accordingly. K+ ions for example, are at equilibrium across the plasma membrane even though they are 30-fold more concentrated inside the cell. the difference in concentration is balanced by the membrane potential, which is more negative on the inside. The membrane potential opposes the movement of cations to the outside of the cell.
Only the molecule NaCl is possible.
No. For equilibrium, the SUM OF ALL FORCES acting on an object must be zero, and that is not possible with a single (non-zero) force.Note: For equilibrium, the sum of all torques on an object must ALSO be zero.
all reactions are equilibrium
This is possible because electrical charges (positive or negative) are non-uniform distributed in the molecule.
yes. Equilibrium can either be static i.e no movement or dynamic i.e movement is allowed. The main determining factor for equilibrium is that all forces acting at a point or points add up to zero.
Supersaturated = Being more concentrated than normally possible and therefore not in equilibrium.