ing 5) n, It t (b) the number of states accessible to the reservoir now, (c) the probability, to an overall multiplicative constant factor, that the small system is in the one state that takes AE, AV, AN from the reservoir 2. Consider a small system that is interacting with a reservoir at temperature 400 K, pressure 108 Pa, and chemical potential -0.3 eV. (a) To go from state 1 to state 2, the small system must take an additional 0.03 eV of energy and 10-29 m³ of volume from the reservoir. How many times more probable is it for the small system to be in state 1 than state 2? (b) To go from state 1 to state 3 the small system must take 0.4 eV of energy and one particle (but no extra volume) from the reservoir. How many times more probable is it that the small system is in state 1 than state 3? (c) To go from state 1 to state 4, the small system must take no energy but one particle and 10-27m³ of volume from the reservoir. How many times more probable is it that the small system is in state 1 than state 4? Section C 3. A certain very delicate organic molecul