Related Formula
F = η A (dv)/(dy)$$F = \eta A \frac{dv}{dy}$$
Surface Tension = (F)/(l)$$\text{Surface Tension} = \frac{F}{l}$$
L = mvr$L = mvr$
K.E = (1)/(2) I ω²$$K.E = \frac{1}{2} I \omega^2$$
Core Logic
Let us determine the dimensional formula for each quantity sequentially:
A. Coefficient of viscosity (η$\eta$):
Using F = η A (dv)/(dy)$F = \eta A \frac{dv}{dy}$, we have:
[M L T⁻²] = η [L²] [T⁻¹]$$[M L T^{-2}] = \eta [L^2] [T^{-1}]$$
η = [M L⁻¹ T⁻¹] ⇒ (III)$$\eta = [M L^{-1} T^{-1}] \Rightarrow \text{(III)}$$
B. Surface Tension (S.T.):
S.T = (F)/( ) = [M L T⁻²][L] = [M L⁰ T⁻²] ⇒ (IV)$$\text{S.T} = \frac{F}{\ell} = \frac{[M L T^{-2}]}{[L]} = [M L^0 T^{-2}] \Rightarrow \text{(IV)}$$
C. Angular momentum (L):
L = mvr = [M] [L T⁻¹] [L] = [M L² T⁻¹] ⇒ (II)$$L = mvr = [M] [L T^{-1}] [L] = [M L^2 T^{-1}] \Rightarrow \text{(II)}$$
D. Rotational kinetic energy (K.E.):
K.E = (1)/(2) I ω² = [M L² T⁻²] ⇒ (I)$$\text{K.E} = \frac{1}{2} I \omega^2 = [M L^2 T^{-2}] \Rightarrow \text{(I)}$$
Step 1: Final Matching
Matching the derived dimensional formulas:
A arrow$\rightarrow$ III
B arrow$\rightarrow$ IV
C arrow$\rightarrow$ II
D arrow$\rightarrow$ I
Pattern Recognition
Kinetic energy (whether translational or rotational) always carries the dimension of Work: [M L² T⁻²]$[M L^2 T^{-2}]$. Surface tension is force per unit length, dropping the L$L$ term. Viscosity commonly includes L⁻¹$L^{-1}$.
Chapter Mix
Class 11 Physics: Units and Measurements