If velocity \vec{v} , acceleration \hat{A} and force f are chosen as fundamental quantities, then the dimensional formula of angular momentum in terms of \nu, A and f would be
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L, v', A', F' \(\Rightarrow\) \(\frac{1}{kv^{r}A^{r}F^{r}}\)
Putting the dimensions in the above relation
\(\left[ML^{2}T^{-2}\right] = k\left[L T^{-1}\right]^{x}\left[L T^{-2} y\right]\left[ML T^{-2}\right]^{z}\)
⇒ ⇒ \(\left[ M L^{2} T^{-1} \right] = k \left[ M^{2} L^{x+v+2} T^{x} y^{-2} \right]\)
Comparing the powers of M, L and \tau
z = 1 …(i)
x + y + z = 2 … (ii)
-x - 2y - 2z = -1 … (iii)
On solving (i), (ii) and (iii) \(x \quad 3y \quad -2z \quad 1\)
So dimension of l in terms of \nu, A and \(\int\)
\(\left[L\right] = \left[F V^{2} A^{-2}\right]\)
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