In two systems of relations among velocity, acceleration and force are
respectively \(v_{2}=\frac{\alpha^{2}}{\beta} v_{1}\), \(a_{2}=\alpha \beta
a_{1}\) and \(F_{2}=\frac{F_{1}}{\alpha \beta}\). If \(\alpha\) and \(\beta\) are
constants then relations among mass, length and time in two systems are
(a) \(M_{2}=\frac{\alpha}{\beta} M_{1}, L_{2}=\frac{\alpha^{2}}{\beta^{2}}
L_{1}, T_{2}=\frac{\alpha^{3} T_{1}}{\beta}\)
(b) \(M_{2}=\frac{1}{\alpha^{2} \beta^{2}} M_{1},
L_{2}=\frac{\alpha^{3}}{\beta^{3}} L_{1}, T_{2}=T_{1}
\frac{\alpha}{\beta^{2}}\)
(c) \(M_{2}=\frac{\alpha^{3}}{\beta^{3}} M_{1},
L_{2}=\frac{\alpha^{2}}{\beta^{2}} L_{1}, T_{2}=\frac{\alpha}{\beta} T_{1}\)
(d) \(M_{2}=\frac{\alpha^{2}}{\beta^{2}} M_{1}, L_{2}=\frac{\alpha}{\beta^{2}}
L_{1}, T_{2}=\frac{\alpha^{3}}{\beta^{3}} T_{1}\)