Transcribed Image Text: ### Flow Analysis Through a Pipe System
The provided diagram (Fig. P3.18) illustrates a pipe system where gasoline flows through three different sections. The flow enters the system at section 1 and exits through two branches, sections 2 and 3. The objective is to determine the average velocity at section 3 and the direction of the flow at this section.
#### Problem Statement:
- **Incoming Flow:**
- Section 1 has a volumetric flow rate of \(0.5 \, \text{m}^3/\text{s}\).
- **Outgoing Flow:**
- Section 2 has an average velocity of \(12 \, \text{m}/\text{s}\).
- **Pipe Diameters:**
- Diameter at section 1 (\(D_1\)) is not given but is integral to determining flow rates.
- Diameter at section 2 (\(D_2\)) is \(18 \, \text{cm}\).
- Diameter at section 3 (\(D_3\)) is \(13 \, \text{cm}\).
#### Diagram Description:
- The diagram shows a primary pipe (section 1) that splits into two branches: section 2 (top branch) and section 3 (bottom branch).
- The flow direction in sections 2 and 3 is indicated by arrows pointing outwards, implying that the gasoline exits the system through these branches.
### Calculations:
To find the average velocity at section 3 (\(V_3\)) and determine whether the flow is in or out, we use the principle of conservation of mass for incompressible fluids. The total volumetric flow rate entering the system must equal the total flow rate exiting the system.
1. **Flow Rate Calculation for Section 2:**
- Flow rate at section 2 (\(Q_2\)) can be calculated using the formula:
\[
Q_2 = A_2 \cdot V_2
\]
- Where, \(A_2\) is the cross-sectional area and \(V_2\) is the velocity.
- The cross-sectional area (\(A_2\)) can be determined from the diameter (\(D_2\)):
\[
A_2 = \pi \left(\frac{D_2}{2}\right)^2 = \pi \left(\frac{18 \,
Behavior of fluids (liquids and gases) when subjected to external forces.
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