\( 2v \)
\( 4v \)
To solve the problem, we need to use the principle of conservation of mass, specifically the equation of continuity for incompressible fluids, which states that the product of the cross-sectional area of the tube and the velocity of the fluid flow through that area is a constant. Mathematically, it is represented as:
\( A_1 v_1 = A_2 v_2 \)
where:
Given the radii:
Substituting the areas into the continuity equation:
\( \pi r^2 \cdot v = \frac{\pi r^2}{4} \cdot v_2 \)
The \( \pi r^2 \) terms cancel out, leaving:
\( v = \frac{v_2}{4} \)
Rearranging to solve for \( v_2 \), we find:
\( v_2 = 4v \)
Therefore, the speed of water in the second tube is \( 4v \).
For an incompressible fluid moving through a tube whose cross-section changes, the volume flow rate must stay the same everywhere along the tube: \( A_1v_1 = A_2v_2 \). Since the cross-sectional area of a tube scales as the square of its radius, this can be rewritten purely as a ratio of radii:
\[ \frac{v_2}{v_1} = \frac{A_1}{A_2} = \left(\frac{r_1}{r_2}\right)^2 \]Here \( r_1 = r \) and \( r_2 = r/2 \), so \( r_1/r_2 = 2 \), giving:
\[ \frac{v_2}{v_1} = 2^2 = 4 \quad\Rightarrow\quad v_2 = 4v \]Checking each option against this ratio:
The correct answer is \( 4v \).