The Boltzmann Distribution Law(2) E More particles have low energy kT more arrangements that way hight.Q= connection between microscopic models macroscopic thermodynamic properties U=kT(OIng and S=kIng+hp/ aIn Q OT medium t- Q= number of states effectively accessible to system Q=∑ep E teEn/kr -Et/kr kT I+e-2/kT E T→+∞0→→0→0>1+1+1+..+1=t low T RTThe Boltzmann Distribution Law (2) ƒ Q ≡ number of states effectively accessible to system E low T E high T E medium T ƒ Q ≡ connection between microscopic models & macroscopic thermodynamic properties and ƒ More particles have low energy: more arrangements that way