For gaseous state, if most probable speed is denoted by `C^(**)` average speed by `barC` and root square speed by `C`, then for a large number of molecules, the ratios of these speeds are
A. `C^(**): bar(C ) : C =1.225:1.128:1`
B. `C^(**): bar(C ) : C =1.128:1.225:1`
C. `C^(**): bar(C ) : C =1:1.128:1.225`
D. `C^(**): bar(C ) : C =1:1.225:1.128`