# Knowledgebase Guide ## Overview The **Knowledgebase** is a reference library of propellants, materials, and engineering equations. It provides the properties needed for calculations in the Solver, Engine Designer, and Rocket Designer. ## Structure The knowledgebase is organized into four categories: 1. **Fuels & Oxidizers** — Propellant properties 2. **Ablative Materials** — Thermal protection 3. **Structural Materials** — Engine & tank construction 4. **Equations** — Mathematical references --- ## Fuels & Oxidizers ### What are They? **Fuel**: Hydrocarbon or hydrogen source - Examples: RP-1 (kerosene), methane, hydrogen **Oxidizer**: Oxygen source - Examples: Liquid oxygen (LOX), nitrogen tetroxide (N2O4) ### Key Properties Each propellant entry contains: **Chemical Properties:** - Molecular formula (e.g., O₂ for oxygen) - Molecular weight (g/mol) - Density (kg/m³) **Combustion Properties:** - **Adiabatic flame temperature (Tc)** — peak temperature of combustion (K) - Higher Tc = higher Isp - Example: LOX/RP-1 ≈ 3750 K, LOX/LH2 ≈ 3900 K - **Expansion ratio (gamma, γ)** — specific heat ratio - γ = Cp / Cv - Affects nozzle performance - LOX/RP-1: γ ≈ 1.25, LOX/LH2: γ ≈ 1.26 - **Characteristic velocity (c*)** — ideal nozzle exit velocity - Fundamental property of propellant - Used to estimate Isp **Performance Metrics:** - **Specific impulse (vacuum, Isp_vac)** — seconds - Higher = better - Example: LOX/RP-1 ≈ 310–320 s, LOX/LH2 ≈ 450 s - **Specific impulse (sea level, Isp_sl)** — reduced due to ambient pressure - Lower than vacuum value - Example: LOX/RP-1 ≈ 260 s at sea level **Mixture Ratio:** - **O/F ratio** — oxidizer mass per fuel mass - Example: LOX/RP-1 optimal ≈ 2.5–2.8 - Higher ratio = more oxygen = higher T but lower mass fraction - Lower ratio = more fuel = lower T but better mass fraction ### Common Propellant Pairs | Fuel | Oxidizer | Isp (s) | Tc (K) | γ | Notes | |------|----------|---------|-------|-------|-------| | RP-1 | LOX | 310 | 3750 | 1.25 | Space-proven, storable | | Methane | LOX | 330 | 3900 | 1.24 | Better impulse than RP-1 | | Hydrogen | LOX | 450 | 3900 | 1.26 | Best impulse, cryogenic, low density | | MMH | N2O4 | 290 | 3400 | 1.20 | Storable, hypergolic (ignites on contact) | | Hydrazine | N2O4 | 310 | 3700 | 1.24 | Toxic but storable, high density | ### Storage Types **Cryogenic:** - Requires refrigeration - LOX, LH2, LN2, LCH4 - Higher energy density - Complex ground support needed **Storable (Room Temperature):** - RP-1, Methane (marginally), MMH, Hydrazine - No cryogenic handling needed - Lower energy density than cryo - Easier integration **Hypergolic:** - Ignites spontaneously on contact (fuel + oxidizer) - No ignition system needed - Toxic, corrosive, more expensive - Examples: MMH/N2O4, Hydrazine/N2O4 ### Selection Criteria **High Performance** → LOX/LH2 (Isp 450 s, but cryogenic complexity) **Best Balance** → LOX/RP-1 (Isp 310 s, storable, proven) **Storable Only** → MMH/N2O4 (Isp 290 s, no cryo needed) **Simple & Solid** → RP-1/LOX or Methane/LOX --- ## Ablative Materials ### Purpose Ablative materials line the rocket engine chamber to withstand: - **High temperature** (combustion products: 3500+ K) - **High pressure** (200+ bar) - **Erosion** from hot gas flow ### Key Properties Each ablative material entry contains: **Mechanical Properties:** - Density (kg/m³) - Tensile strength (MPa) - Compressive strength (MPa) **Thermal Properties:** - Specific heat (J/kg·K) - Thermal conductivity (W/m·K) - Melting point (K) **Erosion Properties:** - **Base erosion rate** (inch/s @ 300 psi reference pressure) - Ablative material mass removed per unit time - Higher rate = thicker liner needed - Example: PAXS ≈ 0.025 in/s - **Pressure exponent (n)** — power-law sensitivity to pressure - `rate(P) = base_rate × (P / P_ref)^n` - Lower n = less pressure-sensitive (better for high P) - Example: PAXS n = 0.38, KFSI n = 0.35 **Application Notes:** - Where used: chamber, nozzle, injector - Temperature limits - Compatibility with propellants ### Material Classes **Composites (Rigid):** - PAXS (polyester + glass) — n = 0.38 - Common, cost-effective - Moderate erosion rate - Max temp ~2000 K - KFSI (silica + phenolic) — n = 0.35 - Better than PAXS - Lower erosion rate - Higher temp capability - More expensive - Carbon-Phenolic — n = 0.32 - Excellent thermal performance - Very low erosion rate - Very expensive - Used on high-end engines **Elastomers (Flexible):** - ZIRCONIA (zirconia + silicone) — n = 0.48 - Flexible (less brittle) - Higher erosion rate - Absorbs vibration - Lower cost than phenolics - Butyl Rubber — n = 0.50 - Very flexible - High erosion rate - Used for low-pressure applications ### Pressure Exponent Explanation The power law `rate ∝ P^n` comes from **regression rate burning**: - Composites: n ≈ 0.3–0.4 - Erosion driven by thermal decomposition - Less pressure-dependent - Preferred for high-pressure engines - Elastomers: n ≈ 0.4–0.5 - Erosion driven by shear stress - More pressure-dependent - OK for moderate pressures **High Pressure (>1000 psi):** Use composite with low n **Moderate Pressure (500 psi):** Elastomer acceptable **Low Pressure (<300 psi):** Elastomer preferred (lower cost) ### Selection Guidance | Application | Material | Reason | |-------------|----------|--------| | High-perf liquid rocket | KFSI or Carbon-Phenolic | Low erosion rate, high pressure capable | | Medium-perf liquid | PAXS | Good balance, cost-effective | | Hybrid rocket | KFSI (fuel grain liner) | Low ablation to preserve geometry | | Solid rocket | Composite | Erosion from particles & hot gas | | Low-cost experiment | Butyl or PAXS | Adequate performance, lowest cost | --- ## Structural Materials ### Purpose Structural materials form the engine chamber and rocket tanks. They must: - Withstand internal pressure (hoop stress) - Resist corrosion from propellants - Perform at operating temperature - Balance weight vs. strength ### Key Properties Each structural material entry contains: **Mechanical Properties:** - **Yield strength** (MPa) — stress at which permanent deformation begins - Higher = thinner walls possible = lighter - Example: Aluminum 6061-T6: 275 MPa, Inconel 718: 1240 MPa - **Young's modulus** (GPa) — stiffness - Higher = less deflection (stronger) - **Density** (kg/m³) — weight per volume - Lower = lighter vehicle - Example: Al: 2700, Ti: 4430, SS: 8000 **Thermal Properties:** - Melting point (K) — temperature limit - Coefficient of thermal expansion (CTE) - Thermal conductivity **Other:** - Cost (relative) - Machinability - Availability ### Material Comparison | Material | Density | Yield | T_melt | Cost | Best For | |----------|---------|-------|--------|------|----------| | Al 6061-T6 | 2700 | 275 | 933 | 1× | Prototype, pressure-fed | | SS 304 | 8000 | 215 | 1726 | 3× | Corrosion resistance | | Inconel 718 | 8190 | 1240 | 1600 | 10× | High-performance engines | | Ti-6-4 | 4430 | 880 | 1941 | 15× | Lightweight, space | | CFRP | 1600 | 600+ | 700 | 20× | Lowest weight | ### Hoop Stress Calculation For cylindrical pressure vessels: ``` σ_hoop = (P × r) / t ``` Setting equal to yield with safety factor: ``` t = (P × r) / (σ_yield / SF) ``` Higher yield strength → thinner walls → lighter mass ### Material Selection **Pressure-Fed Engine (200+ bar, chamber):** - **Inconel 718** — withstands high pressure & heat - **Titanium** — lighter alternative - **Aluminum** — cheap but needs cooling design **Rocket Tanks (20–50 bar):** - **Aluminum 6061** — standard, proven, affordable - **Titanium** — if weight critical - **CFRP** — lowest weight, highest cost **Low-Pressure Systems:** - **Aluminum** — sufficient, cheapest - **Stainless Steel** — if corrosion concern --- ## Equations Reference ### Fundamental Relations **Thrust (momentum equation):** ``` F = ṁ · Ve + (Pe - Pa) · Ae ``` - ṁ = mass flow rate - Ve = exit velocity - Pe = exit pressure - Pa = ambient pressure - Ae = exit area **Specific Impulse:** ``` Isp = Ve / g0 (vacuum) Isp = (Ve - (Pe - Pa) / ṁ · Ae) / g0 (sea level) ``` - g0 = 9.81 m/s² (gravitational acceleration) **Rocket Equation (Tsiolkovsky):** ``` ΔV = Isp · g0 · ln(m_initial / m_final) ``` - ΔV = velocity change (delta-v) - m_initial = wet mass - m_final = dry mass ### Isentropic Flow (Nozzle Design) **Temperature at exit:** ``` Te / T0 = (Pe / P0)^((γ-1)/γ) ``` **Density at exit:** ``` ρe / ρ0 = (Pe / P0)^(1/γ) ``` **Mach number from area ratio:** ``` A / A* = (1/M) · [(2/(γ+1)) · (1 + (γ-1)/2 · M²)]^((γ+1)/(2(γ-1))) ``` - A* = throat area - A = arbitrary section area - M = Mach number - (requires numerical inversion via bisection) **Characteristic velocity:** ``` c* = √[2 · (γ+1)/(γ-1) · R · T0 · (2/(γ+1))^((γ+1)/(γ-1))] ``` ### Thrust Coefficient ``` CF = √[2γ²/(γ-1) · (2/(γ+1))^((γ+1)/(γ-1)) · (1 - (Pe/P0)^((γ-1)/γ))] + (Pe - Pa)/(P0) · (Ae/At) ``` ### Chamber Thermodynamics **Energy balance (no losses):** ``` Cp · (T0 - Te) = Ve² / 2 ``` - Cp = specific heat at constant pressure **Chemical equilibrium:** Determine T0, γ from propellant properties and stoichiometry (computed via NASA CEA code or thermodynamic tables) ### Drag & Atmosphere **Drag force:** ``` Fd = 0.5 · ρ · v² · Cd · A ``` - ρ = air density (depends on altitude) - v = velocity - Cd = drag coefficient (~0.25 for rockets) - A = reference area **US Standard Atmosphere (piecewise):** ``` T(h) = T0 - L·h (troposphere, 0–11 km) P(h) = P0 · (T(h)/T0)^(-g/(R·L)) ρ(h) = ρ0 · (T(h)/T0)^(-(g/(R·L) + 1)) ``` - L = lapse rate ≈ 6.5 K/km - R = gas constant ### Hoop Stress (Pressure Vessels) **Thin-walled cylinder:** ``` σ_hoop = P·r / t ``` With safety factor: ``` t = P·r / (σ_yield / SF) ``` Mass: ``` m = 2π · r · t · L · ρ (cylinder) m = 4π · r² · t · ρ (hemispherical dome) ``` ### Mass Fraction **Payload fraction:** ``` fp = m_payload / m_wet ``` **Structure fraction:** ``` fs = m_structure / m_wet ``` **Propellant fraction:** ``` fp = m_propellant / m_wet ``` Sum: `fp + fs + fpayload = 1` Typical rockets: `fs = 0.10–0.20` (10–20%) --- ## Using Knowledgebase in Design ### Importing Propellant Properties 1. **Solver**: Drag `chamberTemperature`, `expansionGamma` onto workspace 2. Check knowledgebase for propellant pair (LOX + RP-1) 3. Enter T0 from knowledgebase → solver computes Isp 4. Verify with reference Isp in database ### Cross-Checking Ablation 1. **Engine Design**: Select PAXS ablative 2. **Check Pressure Exponent**: 0.38 (from knowledgebase) 3. Verify erosion rate correction is applied 4. Compare remaining thickness to safety margin (>0.5 inch) ### Material Trade-Studies 1. **Rocket Design**: Compare materials - Aluminum: 1000 kg tanks - Titanium: 600 kg tanks (lighter, more expensive) - CFRP: 350 kg tanks (lightest, most expensive) 2. Use mass to compute TWR, delta-v 3. Pick best balance for mission --- ## Future Enhancements - **User contributions**: Allow adding new materials/propellants - **Temperature corrections**: Adjust properties with temperature - **Material compatibility**: Show fuel/material interactions - **Cost database**: Include material & propellant costs - **References**: Link to papers & technical data sources - **Lookup plots**: Interactive charts (Isp vs. O/F, etc.) --- ## References - NASA SP-273: Liquid Rocket Engine Combustion Instability. - Huzel, D. K., & Huang, D. H. (1992). Modern engineering for design of liquid-propellant rocket engines. AIAA. - Rocket Propulsion Elements (8th ed.). Sutton & Biblarz. - US Standard Atmosphere 1976. NASA TM-X-74335. - CEA (Chemical Equilibrium with Applications). NASA Glenn Research Center. --- **Last Updated**: 2025-02 | **Status**: Current