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エネルギー授受を伴うベルヌーイの式【式(3.17)】
添字の数値は管路断面位置を表す.
選択肢
(1) | \(\Large p_2\) | (2) | \(\Large g h_1\) | (3) | \(\LARGE \frac{\rho {v_1}^2}{2}\) | (4) | \(\LARGE \frac{{v_2}^2}{2 g}\) | (5) | \(\Large p_1\) | (6) | \(\LARGE \frac{p_1}{\rho g}\) |
(7) | \(\Large g h_2\) | (8) | \(\LARGE \frac{\rho {v_2}^2}{2}\) | (9) | \(\LARGE \frac{p_1}{\rho}\) | (10) | \(\LARGE \frac{p_2}{\rho g}\) | (11) | \(\Large e_T\) | (12) | \(\LARGE \frac{p_2}{\rho}\) |
(13) | \(\LARGE \frac{e_P}{g}\) | (14) | \(\LARGE \frac{{v_1}^2}{2 g}\) | (15) | \(\LARGE \frac{{v_2}^2}{2}\) | (16) | \(\Large h_2\) | (17) | \(\Large \rho g h_1\) | (18) | \(\Large h_1\) |
(19) | \(\Large e_P\) | (20) | \(\Large \rho e_P\) | (21) | \(\LARGE \frac{{v_1}^2}{2}\) | (22) | \(\Large \rho g h_2\) | (23) | \(\LARGE \frac{e_T}{g}\) | (24) | \(\Large \rho e_T\) |