In an effort to elucidate the origin of stimuli-responsive (T
SR) transitions and correlate them to the glass transition temperature (T
g), poly(N-acryloyl-N′-propylpiperazine-co-2-ethoxyethyl methacrylate) (p(AcrNPP/EEMA)), poly(N-vinylcaprolactam-co-n-butyl acrylate) (p(VCl/nBA)), poly(N-isopropyl methacrylamide-co-n-butyl acrylate) (p(NIPMAm/nBA)), and poly(2-(N,N′-dimethylamino)ethyl methacrylate-co-n-butyl acrylate) (p(DMAEMA/nBA)) colloidal dispersions were synthesized, which upon coalescence form solid films. These studies showed that molecular rearrangements responsible for the T
SR transitions are attributed to the backbone buckling and collapse of stimuli-responsive components. Based on empirical data, the relationship between T
g and T
SR was established: log(V
1/V
2) = (P
1(T
SR − T
g))/(P
2 + (T
SR − T
g)), where the V
1 and V
2 are the copolymer total volumes below and above the T
SR, respectively, T
g is the glass transition temperature of the copolymer, and P
1 and P
2 are the fraction of the free volume (f
free) at T
g (P
1) and (T
g,midpoint − T
SR)50/50) for each random copolymer (P
2), respectively. This relationship can be utilized to predict the total volume changes as a function of T
SR − T
g for different copolymer compositions. To our best knowledge, this is the first study that provides the relationship between the T
SR, T
g, free volume, chain mobility, and dimensional changes in stimuli-responsive random copolymer networks.