Aerospace Engineer
Aerothermodynamics & Propulsion Systems
B.S. Aerospace Engineering — UC San Diego. Specialized in aerothermodynamics with hands-on experience in CFD simulation, experimental aerodynamics, propulsion analysis, and autonomous vehicle design. Bilingual. Based in National City, CA.
Engineering Work
Modeled an innovative vortex cooling concept for liquid rocket engines using Ansys Fluent. Cryogenic propellants are injected tangentially to generate a swirling vortex flow that forms a protective thermal film along the nozzle wall — isolating the chamber liner from extreme combustion temperatures without active cooling hardware.
YZ velocity contour — blue (low velocity) in chamber transitions to red (>650 m/s) at nozzle exit. The sharp gradient confirms efficient vortex-driven acceleration.
Surface velocity vectors colored by magnitude. The swirling pattern at the injector ports confirms vortex formation; high-velocity orange vectors at the nozzle throat show peak flow acceleration.
Polyhedral CFD mesh generated in Ansys Fluent 2024 R1. Finer boundary-layer cells (teal) along chamber walls capture near-wall thermal gradients critical to evaluating the vortex cooling film.
Full CFD simulation video showing transient vortex development, chamber pressure buildup, and steady-state flow through the nozzle.
A full-featured MATLAB tool that reads aircraft definitions from a structured Excel input file and computes aerodynamic performance, structural loads, and FAR Part 23 flight envelope data at both sea level and altitude. Applied to a modified Cessna 172R (350 hp engine upgrade) as a final project for SE160A at UC San Diego.
V-n diagram recreated from actual MATLAB output values. Blue curves show the maneuver envelope (stall boundary + structural limits). Red lines show the FAR 23 gust diamond at 50 ft/s (cruise) and 25 ft/s (dive). Dashed blue shows flaps-deployed envelope.
Data flows from the Excel input sheet through four MATLAB script sections (Parts A–D). Each section reads shared workspace variables, so changing the input propagates automatically to all outputs.
%% Gust alleviation factor (FAR Part 23) mu2 = 2*Weight(8) / (rhoa*g*(S/144) ... *(Croot+Ctip)/24*dCL*(180/pi)); Kg2 = 0.88*mu2 / (5.3 + mu2); %% Gust load factors at cruise and dive speed LfG(1) = 1 + Kg2*(.5*rhoa*U(1)*(S/144) ... /Weight(8)*dCL*(180/pi))*Vk4(5)*K2Fps; LfG(3) = 1 - Kg2*(.5*rhoa*U(1)*(S/144) ... /Weight(8)*dCL*(180/pi))*Vk4(7)*K2Fps; %% Wing lift, drag, structural loads at each V-n point for i = 1:8 Lt4(i) = (Ma4(i) + Weight(8)*Lf4(i) ... *(Arcrft_CG(8)-c4wing)/12) ... / ((c4_hs-c4wing)/12); Lw4(i) = Weight(8)*Lf4(i) - Lt4(i); %% Rotation matrix: aero → structural frame T = [cosd(alpha4(i)) sind(alpha4(i)); ... -sind(alpha4(i)) cosd(alpha4(i))]; Resultant4(:,i) = T * [Lw4(i) - Lf4(i)*Wwing; ... Dragwing4(i)]; end %% Power lapse correction for altitude Rrho = rhoa / rho; Power4a = Power4 .* (Rrho - (1-Rrho)/7.55).^(-1);
Excerpt from Part C of the MATLAB script. The 2×2 rotation matrix T transforms wing lift and drag from the aerodynamic (wind) frame into the structural (body) frame — essential for correct spar and rib load calculations. Power lapse at altitude uses an empirical correction factor for propeller efficiency.
| Condition | Speed (kts) | n | Wing Lift (lb) | Power Req. (hp) |
|---|---|---|---|---|
| Stall (flaps up) | 51 | 1.0 | 2,396 | 45 |
| Cruise (VNO) | 126 | 1.0 | 2,516 | 146 |
| PHAA (max maneuver) | 99.4 | +3.8 | 9,105 | 331 |
| NHAA (max neg. maneuver) | 62.9 | -1.52 | -3,570 | 81 |
| Gust +50 ft/s (cruise) | 126 | +3.99 | 9,608 | 364 |
| Dive (VNE) | 160 | 3.8 | 9,247 | 437 |
All values from the Excel output file generated by the MATLAB tool. The gust at cruise speed (n = 3.99) exceeds the structural maneuver limit (n = 3.8), making it the critical design load case for wing spar sizing.
Designed, built, and tested a rotary-wing lander concept for planetary bodies with thin atmospheres. The vehicle uses passive blade pitch geometry to maintain a stable rotation rate and constant descent velocity — no active power source required for the rotor. An onboard camera captures imagery throughout descent.
Conducted experimental lift and drag measurements on a wing section across multiple angles of attack in a subsonic wind tunnel. Operated force balance instrumentation, extracted raw sensor data, and post-processed results to derive aerodynamic coefficient curves.
Capabilities
Background
I'm an aerospace engineer based in National City, CA, with a B.S. from UC San Diego specializing in aerothermodynamics. My technical foundation spans CFD simulation, propulsion systems, experimental aerodynamics, and embedded systems design.
My most technically involved project was a CFD simulation of a vortex-cooled rocket engine — an innovative approach where propellants are injected tangentially to create a swirling flow that keeps a cryogenic film on the nozzle wall, passively protecting it from combustion temperatures. The simulation validated both vortex stability and thermal performance.
I also built a physical autorotation planetary lander — a rotary-wing vehicle that descends at a stable rate with no active rotor power, integrated with a camera system and Arduino-based control logic, all within strict mass and volume constraints.
I'm fluent in both English and Spanish and am actively seeking an entry-level or apprentice engineering role where I can contribute to real hardware and grow my applied experience.
Get in Touch
I'm actively looking for entry-level or apprentice positions in aerospace, propulsion, MRO, or defense engineering. I'd love to hear from you.