The given equation is a modified form of Bernoulli’s equation:
\[ P + \frac{A}{B t^2} + \rho g (h + Bt) + \frac{1}{2}\rho v^2 = \text{constant} \]
Since this is a Bernoulli-type equation, every term must have the dimensions of pressure.
\[ [P] = [ML^{-1}T^{-2}] \]
This term must have dimensions of pressure:
\[ \frac{[A]}{[B][T^2]} = [ML^{-1}T^{-2}] \]
Rearranging:
\[ [A] = [B]\,[T^2]\,[ML^{-1}T^{-2}] \]
The quantity inside the brackets must have dimensions of length:
\[ [h] = [Bt] = L \]
Since \( t \) has dimensions \( [T] \), we get:
\[ [B] = [LT^{-1}] \]
Substitute \( [B] = [LT^{-1}] \) into the expression for \( [A] \):
\[ [A] = [LT^{-1}] \times [T^2] \times [ML^{-1}T^{-2}] \]
Simplifying:
\[ [A] = [ML^0T^{-1}] \]
All terms are dimensionally consistent with pressure.
\[ [A] = ML^0T^{-1}, \qquad [B] = LT^{-1} \]