To solve this problem, we need to apply the principle of continuity for fluid flow. The principle of continuity states that for an incompressible fluid flowing through a pipe of varying diameter, the product of the cross-sectional area and the velocity of the fluid at any point in the pipe is constant. Mathematically, this is represented as:
A_1V_1 = A_2V_2where A_1 and A_2 are the cross-sectional areas at points 1 and 2, and V_1 and V_2 are the velocities at those points.
The areas A_1 and A_2 can be calculated using the formula for the area of a circle:
A = \pi \left(\frac{d}{2}\right)^2Given:
First, calculate A_1 and A_2:
Using the continuity equation A_1V_1 = A_2V_2, we can express the velocity ratio \frac{V_2}{V_1} as:
\frac{V_2}{V_1} = \frac{A_1}{A_2} = \frac{10.24\pi}{5.76\pi}Simplifying gives:
\frac{V_2}{V_1} = \frac{10.24}{5.76} = \frac{64}{36} = \frac{16}{9}Therefore, the inverse ratio, or the ratio of the minimum to the maximum velocity, is:
\frac{V_1}{V_2} = \frac{9}{16}Thus, the correct answer is \frac{9}{16}, which matches the given correct answer.
Water flows through a horizontal tube as shown in the figure. The difference in height between the water columns in vertical tubes is 5 cm and the area of cross-sections at A and B are 6 cm\(^2\) and 3 cm\(^2\) respectively. The rate of flow will be ______ cm\(^3\)/s. (take g = 10 m/s\(^2\)). 