Step 1: Understanding the Concept:
Dimensional analysis and Buckingham's $\pi$-theorem: if a physical phenomenon involves $n$ independent physical variables expressed in $m$ fundamental dimensions ($M, L, T, heta$), the relationship can be expressed as a function of exactly $(n - m)$ independent dimensionless $\pi$-groups.
Key Formula or Approach:
\[ \mathbf{Number \text{ } of \text{ } Dimensionless \; \pi\text{-Terms}} = \mathbf{n - m} \quad [n = \text{Total Variables}, \; m = \text{Fundamental Dimensions}] \]
Step 2: Detailed Explanation:
In dimensional analysis, fluid mechanics, and heat transfer modeling (Buckingham's $\pi$-Theorem, Edgar Buckingham 1914):
- Buckingham's Pi Theorem states:
1. If a dimensionally homogeneous equation involves $n$ physical variables (dependent and independent variables, such as velocity, pressure drop, viscosity, diameter, density):
\[ f(q_1, q_2, q_3, \dots, q_n) = 0 \]
2. And these $n$ variables contain $m$ fundamental primary dimensions (such as Mass $M$, Length $L$, Time $T$, Temperature $\theta$):
3. Then the equation can be reformulated and simplified into an equivalent relationship involving exactly (n - m) independent dimensionless groups ($\pi$-terms) (A):
\[ \phi(\pi_1, \pi_2, \dots, \pi_{n-m}) = 0 \]
- (This is the foundational mathematical theorem used to derive the Reynolds number $Re$, Nusselt number $Nu$, and Prandtl number $Pr$ in dairy thermal engineering).
Step 3: Final Answer:
Therefore, the equation will have (n - m) dimensionless groups, corresponding to option (A).