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Water from a tap emerges vertically down...

Water from a tap emerges vertically downwards with an initial spped of `1.0ms^-1`. The cross-sectional area of the tap is `10^-4m^2`. Assume that the pressure is constant throughout the stream of water, and that the flow is steady. The cross-sectional area of the stream 0.15 m below the tap is

A

`5.0 xx 10^(-4)m^(2)`

B

`1.0 xx 10^(-4) m^(2)`

C

`5.0 xx 10^(-5)m^(2)`

D

`2.0 xx 10^(-5)m^(2)`

Text Solution

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The correct Answer is:
To solve the problem, we will use the principles of fluid mechanics, specifically the conservation of energy and the continuity equation. ### Step-by-Step Solution: 1. **Identify Given Values:** - Initial speed of water, \( v_1 = 1.0 \, \text{m/s} \) - Cross-sectional area of the tap, \( A_1 = 10^{-4} \, \text{m}^2 \) - Height below the tap, \( h = 0.15 \, \text{m} \) - Acceleration due to gravity, \( g = 10 \, \text{m/s}^2 \) (assuming standard value) 2. **Apply Conservation of Energy:** The total mechanical energy at the tap (point A) must equal the total mechanical energy at a point 0.15 m below (point B). The potential energy at point A is converted into kinetic energy at point B. The energy equation can be written as: \[ \text{PE}_A + \text{KE}_A = \text{PE}_B + \text{KE}_B \] Where: - \(\text{PE} = \rho g h\) (potential energy) - \(\text{KE} = \frac{1}{2} \rho v^2\) (kinetic energy) At point A: \[ \text{PE}_A = \rho g h + \frac{1}{2} \rho v_1^2 \] At point B (where potential energy is zero): \[ \text{PE}_B = 0 + \frac{1}{2} \rho v_2^2 \] Setting them equal: \[ \rho g h + \frac{1}{2} \rho v_1^2 = \frac{1}{2} \rho v_2^2 \] 3. **Simplify the Equation:** We can cancel \(\rho\) from both sides (assuming it is constant): \[ g h + \frac{1}{2} v_1^2 = \frac{1}{2} v_2^2 \] 4. **Substitute Known Values:** Substitute \(g = 10 \, \text{m/s}^2\), \(h = 0.15 \, \text{m}\), and \(v_1 = 1.0 \, \text{m/s}\): \[ 10 \cdot 0.15 + \frac{1}{2} (1.0)^2 = \frac{1}{2} v_2^2 \] \[ 1.5 + 0.5 = \frac{1}{2} v_2^2 \] \[ 2 = \frac{1}{2} v_2^2 \] 5. **Solve for \(v_2\):** Multiply both sides by 2: \[ 4 = v_2^2 \] Taking the square root: \[ v_2 = 2 \, \text{m/s} \] 6. **Apply the Continuity Equation:** According to the continuity equation: \[ A_1 v_1 = A_2 v_2 \] Rearranging gives: \[ A_2 = \frac{A_1 v_1}{v_2} \] 7. **Substitute Known Values:** \[ A_2 = \frac{10^{-4} \cdot 1.0}{2} = \frac{10^{-4}}{2} = 5 \times 10^{-5} \, \text{m}^2 \] ### Final Answer: The cross-sectional area of the stream 0.15 m below the tap is \( A_2 = 5 \times 10^{-5} \, \text{m}^2 \). ---

To solve the problem, we will use the principles of fluid mechanics, specifically the conservation of energy and the continuity equation. ### Step-by-Step Solution: 1. **Identify Given Values:** - Initial speed of water, \( v_1 = 1.0 \, \text{m/s} \) - Cross-sectional area of the tap, \( A_1 = 10^{-4} \, \text{m}^2 \) - Height below the tap, \( h = 0.15 \, \text{m} \) ...
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