Also, another way of thinking about
Q:
For a system, aA + bB <---> cC + dD, the condition for being at equilibrium is that Rate Fwd = Rate Rev > 0.
For mathematical reasons that we don't deal with, this condition is equivalent to
but this applies only at equilibrium.
We define the equilibrium constant,
K, as the constant value found from this expression. The fraction of concentrations, however, is variable, it changes as the system moves, and so we define it as the reaction quotient,
Q. The condition for a system to be at equilibrium is consequently that
Q =
K, as at that time the concentrations have the values where the system is at equilibrium. Though we teach it backwards, the consequence here is that it follows that
at equilibrium only. If the system is not at equilibrium then
Put another way,
Q is a function of several variables (the concentrations in its expression) and
K is a constant value of that function that happens to have a useful significance, just as I can make an equation for the area of a field based on given information and then seek the value that corresponds to its maximum.
Le Chatelier's Principle disturbances can then be examined as situations where a change has caused (usually) the value of
Q to move away from
K, and the system will shift so as to return to having
Q =
K. This also means that the concentrations at equilibrium that we substitute to find
K are not unique, and there are other combinations of concentrations that will result in
Q equalling
K.