\displaystyle \frac{1}{2}\rho{v_2^2} + p_1 = \frac{1}{2}\rho{v_1^2} + p _2 \\[br]p_1 - p_2 = \frac{1}{2}\rho\left(v_2^2 - v_1^2\right) \\ [br]\partial_t\rho + \nabla\cdot\rho\vec{v} = 0 \\ [br]0 + \oint \rho\vec{v}\cdot{d\vec{s}} = 0 \\ [br]\rho{v_1}{A_1} = \rho{v_2}{A_2} \\ [br]v_1\left(\frac{d_1}{d_2}\right)^2 = v_2 \\ [br]\therefore p_1 - p_2 = \frac{1}{2}\rho{v_1^2}\left(\left(\frac{d_1}{d_2}\right)^4 - 1\right)[br]
\displaystyle \frac{1}{2}\rho{v_2^2} + p_1 = \frac{1}{2}\rho{v_1^2} + p _2 \\[br]p_1 - p_2 = \frac{1}{2}\rho\left(v_2^2 - v_1^2\right) \\ [br]\partial_t\rho + \nabla\cdot\rho\vec{v} = 0 \\ [br]0 + \oint \rho\vec{v}\cdot{d\vec{s}} = 0 \\ [br]\rho{v_1}{A_1} = \rho{v_2}{A_2} \\ [br]v_1\left(\frac{d_1}{d_2}\right)^2 = v_2 \\ [br]\therefore p_1 - p_2 = \frac{1}{2}\rho{v_1^2}\left(\left(\frac{d_1}{d_2}\right)^4 - 1\right)[br]
\displaystyle \frac{1}{2}\rho{v_2^2} + p_1 = \frac{1}{2}\rho{v_1^2} + p _2 \\[br]p_1 - p_2 = \frac{1}{2}\rho\left(v_2^2 - v_1^2\right) \\ [br]\partial_t\rho + \nabla\cdot\rho\vec{v} = 0 \\ [br]0 + \oint \rho\vec{v}\cdot{d\vec{s}} = 0 \\ [br]\rho{v_1}{A_1} = \rho{v_2}{A_2} \\ [br]v_1\left(\frac{d_1}{d_2}\right)^2 = v_2 \\ [br]\therefore p_1 - p_2 = \frac{1}{2}\rho{v_1^2}\left(\left(\frac{d_1}{d_2}\right)^4 - 1\right)[br]
\left(p_1-p_2) + \frac{1}{2}\left(\rho_1v_1^2 - \rho_2v_2^2\right) + \left(\Phi_1-\Phi_2\right) = 0