What would happen to a system at equilibrium if the temperature were changed?
An increase in temperature shifts to the reactant side in a exothermic reaction. In an endothermic reaction, the sift is toward the product side.
Le Chatelier states that a stress that disturbs equilibrium moves to the opposite side in order to release the tension.
Since heat is released in an exothermic reaction, rising temperatures cause the equilibrium to move to the reactant side of the reaction, while falling temperatures cause the reaction to move to the product side.
Since heat is absorbed by the reaction in an endothermic reaction, an increase in temperature will shift to the product side, and a decrease in temperature will shift to the reactant side.
The equilibrium constant will rise with any shifts to the product side and fall with any shifts to the reactant side.
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If the temperature of a system at equilibrium is changed, the equilibrium position will shift to counteract the change in temperature, according to Le Chatelier's principle. If the temperature increases, the equilibrium will shift in the endothermic direction (towards the side of the reaction that absorbs heat) to consume the excess heat. If the temperature decreases, the equilibrium will shift in the exothermic direction (towards the side of the reaction that releases heat) to compensate for the loss of heat.
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When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
When evaluating a one-sided limit, you need to be careful when a quantity is approaching zero since its sign is different depending on which way it is approaching zero from. Let us look at some examples.
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