Given equation:
\[ \left( P + \frac{A^2}{B} \right) + \frac{1}{2} \rho V^2 = \text{constant}, \] where:
1. Dimensions of Pressure \( P \):
Pressure is force per unit area. The dimensions of force are \( MLT^{-2} \), and area has dimensions \( L^2 \). Therefore, the dimensions of pressure are:
\[ [P] = \frac{MLT^{-2}}{L^2} = ML^{-1}T^{-2}. \]
2. Dimensions of \( \frac{A^2}{B} \):
Since the sum \( \left( P + \frac{A^2}{B} \right) \) is equal to a constant, the dimensions of both terms must be the same. Therefore, the dimensions of \( \frac{A^2}{B} \) must be \( ML^{-1}T^{-2} \).
Let’s assume the dimensions of \( A \) and \( B \) are \( [A] = M^xL^yT^z \) and \( [B] = M^pL^qT^r \), respectively. Then, the dimensions of \( \frac{A^2}{B} \) are:
\[ \left[\frac{A^2}{B}\right] = \frac{(M^x L^y T^z)^2}{M^p L^q T^r} = M^{2x-p} L^{2y-q} T^{2z-r}. \]
For the dimensions to be consistent with \( ML^{-1}T^{-2} \), we must have:
3. Dimensions of \( A/B \):
From the above, we can solve for the dimensions of \( A \) and \( B \). After solving, we find that:
\[ \left[ \frac{A}{B} \right] = ML^{-1}T^{-4}. \]
Final Answer: The dimensions of \( \frac{A}{B} \) are \( \boxed{ML^{-1}T^{-4}} \).
Match List-I with List-II.
| List-I (A) Coefficient of viscosity (B) Intensity of wave (C) Pressure gradient (D) Compressibility | List-II (I) [ML-1T-1] (II) [MT-3] (III) [ML-2T-2] (IV) [M-1LT2] |
The equation for real gas is given by $ \left( P + \frac{a}{V^2} \right)(V - b) = RT $, where $ P $, $ V $, $ T $, and $ R $ are the pressure, volume, temperature and gas constant, respectively. The dimension of $ ab $ is equivalent to that of:
The dimensions of a physical quantity \( \epsilon_0 \frac{d\Phi_E}{dt} \) are similar to [Symbols have their usual meanings]


