Give step-by-step solution with explanation and final answer:1. The average specific impulse of a chemical rocket is 360 s. The rocket is in a zero- gravity vacuum flight. Calculate and graph vehicle terminal speed AV for the propellant fraction ¢; that ranges between 0.80 and 0.95.
Question:
Give step-by-step solution with explanation and final answer:
1. The average specific impulse of a chemical rocket is 360 s. The rocket is in a zero-
gravity vacuum flight. Calculate and graph vehicle terminal speed AV for the
propellant fraction ¢; that ranges between 0.80 and 0.95.
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Asked by: Veera manikanta
Created at: 2025-10-04 22:39:52
Asked by: Veera manikanta
Created at: 2025-10-04 22:39:52
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## Problem Restatement
Given- Specific impulse rocket \( I_{sp} = 360 \) s
- Zero-gravity, vacuum flight
- Propellant fraction \( \zeta \) ranges from .80 to .95
**Task**:
Calculate and graph the terminal speed (\( \Delta V \)) as a function of \( \zeta \).
---
## Step 1: Rocket Equation
We use the **Tsiolkovsky Rocket Equation**:
\[
\Delta V = I_{sp} \cdot g_ \cdot \ln\left(\frac{m_}{m_f}\right)
\]
Where:
- \( I_{sp} \) = specific impulse (s)
- \( g_ \) = standard gravity (\( 9.81\,\text{m/s}^2 \))
- \( m_ \) = initial mass (vehicle + propellant)
- \( m_f \) = final mass (vehicle after burning propellant)
---
## Step 2: Express Mass Ratio in Terms of Propellant Fraction
Propellant fraction \( \zeta \):
\[
\zeta = \frac{m_ - m_f}{m_}
\implies m_f = m_ (1 - \zeta)
\]
So,
\[
\frac{m_}{m_f} = \frac{m_}{m_(1 - \zeta)} = \frac{1}{1 - \zeta}
\]
---
## Step 3: Substitute Values
Plug in \( I_{sp} = 360\,\text{s} \), \( g_ = 9.81\,\text{m/s}^2 \):
\[
\Delta V = 360 \times 9.81 \times \ln\left(\frac{1}{1 - \zeta}\right)
\]
\[
\Delta V = 3531.6 \times \ln\left(\frac{1}{1 - \zeta}\right)
\]
\[
\Delta V = 3531.6 \times \left[-\ln(1 - \zeta)\right]
\]
\[
\Delta V = -3531.6 \times \ln(1 - \zeta)
\]
---
## Step 4: Calculate for Given Range
Let's compute a few values for \( \zeta \) between .80 and .95:
| \( \zeta \) | \( \Delta V = -3531.6 \times \ln(1 - \zeta) \) (m/s) |
|:----------:|------------------------------------:|
| .80 | \( -3531.6 \times \ln(.20) = 3531.6 \times 1.6094 = 5687 \) m/s |
| .85 | \( -3531.6 \times \ln(.15) = 3531.6 \times 1.8971 = 6702 \) m/s |
| .90 | \( -3531.6 \times \ln(.10) = 3531.6 \times 2.3026 = 8134 \) m/s |
| .95 | \( -3531.6 \times \ln(.05) = 3531.6 \times 2.9957 = 10576 \) m/s |
---
## Step 5: Graph
Here is the relationship, which you can plot:
\[
\boxed{
\Delta V = -3531.6 \times \ln(1 - \zeta),\quad .80 \leq \zeta \leq .95
}
\]
### Table of Results
| Propellant Fraction (\( \zeta \)) | Terminal Speed (\( \Delta V \), m/s) |
|:----------------:|:-------------------------:|
| .80 | 5687 |
| .85 | 6702 |
| .90 | 8134 |
| .95 | 10576 |
---
### Graph (Description)
- **X-axis:** Propellant fraction (\( \zeta \)), from .80 to .95
- **Y-axis:** Terminal speed (\( \Delta V \)), from 500 to 11000 m/s
- **Shape:** Exponential increase as \( \zeta \) approaches 1
You can plot this in Excel, Python, or any graphing calculator using the above equation.
---
## **Final Answer**
\[
\boxed{
\Delta V = -3531.6 \times \ln(1 - \zeta)
}
\]
For \( \zeta \) between .80 and .95, \(\Delta V\) varies from approximately **5687 m/s to 10576 m/s**. The relationship is nonlinear and can be graphed as described above.
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