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Act like a helpful tutor and exlain me : Give step-by-step solution with explanation and final answer:Question #2 Assume that you have a tapered water fountain pipe, and the water pressure in the engineering building results in 80 psi of pressure at the location of the pressure gauge in Fig. 2. Assume that water flows without viscous effects from the nozzle shown in Fig. 2. Estimate the flowrate in L/s and the height, h in meters, to which the water can reach for your indoor fountain.

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Act like a helpful tutor and exlain me : Give step-by-step solution with explanation and final answer:Uploaded ImageQuestion #2 Assume that you have a tapered water fountain pipe, and the water pressure in the engineering building results in 80 psi of pressure at the location of the pressure gauge in Fig. 2. Assume that water flows without viscous effects from the nozzle shown in Fig. 2. Estimate the flowrate in L/s and the height, h in meters, to which the water can reach for your indoor fountain.

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Asked by: manish kumar
Created at: 2025-09-22 23:39:29

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Let's break down the problem step by step: --- ## **Given Data** - **Pressure at the nozzle:** \( P = 80 \) psi - **Water flows without viscous effects** (Assume ideal fluid) - **Gravity:** \( g = 9.81 \) m/s² - **Water density:** \( \rho = 1000 \) kg/m³ (standard for water) - **Atmospheric pressure at exit** - **Need to find:** - **Flowrate** (L/s) - **Maximum height (\( h \))** water can reach --- ## **Step 1: Convert Pressure Units** Convert psi to Pascals (SI units): \[ 1\,\text{psi} = 6894.76\,\text{Pa} \] \[ P = 80\,\text{psi} \times 6894.76\,\text{Pa/psi} = 551,580.8\,\text{Pa} \] --- ## **Step 2: Use Bernoulli’s Equation** Assume the nozzle exit is open to the atmosphere (so pressure at exit = atmospheric). Bernoulli’s equation between gauge and nozzle exit: \[ P_1 + \frac{1}{2}\rho v_1^2 + \rho g z_1 = P_2 + \frac{1}{2}\rho v_2^2 + \rho g z_2 \] Assume: - Point 1: at gauge (pipe, upstream, large area, velocity \( v_1 \approx 0 \)) - Point 2: at nozzle exit (open to atmosphere, at same height, \( z_1 = z_2 \)) So, \[ P_1 = P_2 + \frac{1}{2}\rho v_2^2 \] Since \( P_2 \) is atmospheric, and \( P_1 \) is the gauge pressure (above atmospheric): \[ P_{\text{gauge}} = \frac{1}{2}\rho v_2^2 \] Solve for \( v_2 \): \[ v_2 = \sqrt{\frac{2 P_{\text{gauge}}}{\rho}} \] \[ v_2 = \sqrt{\frac{2 \times 551,580.8}{1000}} \] \[ v_2 = \sqrt{1103.1616} \] \[ v_2 \approx 33.23\,\text{m/s} \] --- ## **Step 3: Flowrate Calculation** \[ Q = A v_2 \] But the nozzle area (\( A \)) is not given. Typically, you'd need to know the diameter. **If not specified, let's assume a standard small fountain nozzle, say diameter \( d = 1 \) cm = 0.01 m:** \[ A = \frac{\pi d^2}{4} = \frac{\pi (0.01)^2}{4} = 7.854 \times 10^{-5}\,\text{m}^2 \] So, \[ Q = 7.854 \times 10^{-5}\,\text{m}^2 \times 33.23\,\text{m/s} \approx 0.00261\,\text{m}^3/\text{s} \] Convert to L/s (\(1\,\text{m}^3 = 1000\) L): \[ Q \approx 2.61\,\text{L/s} \] --- ## **Step 4: Maximum Height (\( h \))** Use kinematics (projectile motion, vertical): \[ v^2 = 2gh \implies h = \frac{v^2}{2g} \] \[ h = \frac{(33.23)^2}{2 \times 9.81} = \frac{1104.2}{19.62} \approx 56.3\,\text{m} \] --- ## **Final Answers** ### **1. Flowrate** \[ \boxed{2.61~\text{L/s}} \] (for a 1 cm diameter nozzle; use the actual nozzle size if known) ### **2. Maximum Height** \[ \boxed{56.3~\text{m}} \] --- ### **Summary Table** | Quantity | Formula | Value | |------------------|-------------------------------------------------|--------------------| | Exit velocity | \( v = \sqrt{2P/\rho} \) | 33.2 m/s | | Flowrate | \( Q = A v \) | 2.61 L/s (d=1 cm) | | Max height | \( h = v^2/2g \) | 56.3 m | > **Note:** If the nozzle diameter is different, recalculate \( Q \) using \( d \) provided. --- Let me know if you have the nozzle diameter or need more details!

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