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Application of Mathematics Competency

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Principles of Mathematics Competency

Our project involved designing and building air rockets constructed primarily from cardboard (body tube, nose cone, fins) and duct tape, then launched by compressed air. The goal was to achieve maximum height while ensuring stable flight and durability. Challenges included predicting and measuring altitude, accounting for drift, and optimizing designs for minimal drag.

Specific Problem Solved Using Mathematics

Determining the rocket's maximum altitude (apogee).

We used ground-based trigonometry tracking. From a known baseline distance on the ground, we measured the elevation angle to the rocket at its highest point using a clinometer.

Launch Geometry & Tracking Setup

θ h (height) d = 150 ft (baseline, measured by surveyor's wheel) line of sight Ground-Based Trigonometry Tracking (not to scale)

Figure 1 — An observer at a known baseline distance uses a clinometer to measure elevation angle θ to the rocket at apogee.

Math Application: Trigonometry (SOH-CAH-TOA)

Because the rocket travels roughly vertically from the launch pad and the observer stands on flat ground, the launch pad, the observer, and the rocket at apogee form a right triangle. Right-triangle trigonometry gives us the relationship between the known baseline and the unknown altitude.

Opposite = h (height) Adjacent = d (baseline) Hypotenuse θ
SOH — sin θ = Opposite / Hypotenuse
CAH — cos θ = Adjacent / Hypotenuse
TOA — tan θ = Opposite / Adjacent

← This is the ratio we used

  • Opposite (h) — unknown rocket height
  • Adjacent (d) — ground baseline, 150 ft, measured with a surveyor's wheel
  • Angle (θ) — elevation angle measured with a clinometer

Derived Formula

tan θ = h / d

h = d × tan(θ)

h = 150 × tan(θ)

Solving for h by multiplying both sides by d (150 ft).

Height Computations — Recorded Data

Using the 150 ft baseline, we recorded elevation angles at apogee across multiple launches and applied the formula to compute each rocket's maximum height.

Launch Angle θ (°) tan(θ) Baseline d (ft) Height h = d·tan θ (ft)
R1 25° 0.4663 150 ≈ 70 ft
R2 10° 0.1763 150 ≈ 26 ft
R3 20° 0.3640 150 ≈ 55 ft
R7 20° 0.3640 150 ≈ 55 ft
R8 15° 0.2679 150 ≈ 40 ft
R9 15° 0.2679 150 ≈ 40 ft
Observed range 26 – 70 ft

Values cross-referenced with field notebook records. Some angles repeated across launches indicate consistent drag behaviour for a given design iteration.

Field Notebook — Calculations & Sketches

Handwritten engineering notebook showing rocket height calculations, SOH-CAH-TOA work, angle measurements, and scatter plots of height vs. mass and height vs. center of gravity

Handwritten engineering notebook showing angle measurements, tan computations (tan 25° · 150 = Hrocket), distance of CG to nose cone per rocket, and scatter plots analysing height vs. mass and center of gravity.

Rocket designs used as reference during the project

Rocket designs for reference.

Analysis & Engineering Insights

The computed heights (26–70 ft across all launches) established a measurable benchmark for comparing predicted versus actual performance. The trigonometric method gave us an objective, repeatable way to quantify design changes.

Design Flaws Revealed

Launches reaching only 26–40 ft (θ ≤ 15°) correlated with oversized fins that increased drag and damaged nose cones that disrupted laminar airflow, both visible in the notebook's scatter plots.

Iterative Improvement

Trimming fins and reinforcing nose cones pushed angles toward 20–25°, nearly tripling altitude from the lowest runs. Each iteration was justified by the computed h values, making mathematics the direct driver of design decisions.

Drift & Measurement Uncertainty

Horizontal drift meant the true apogee could be slightly off-axis from the baseline, introducing a small cosine error. We mitigated this by positioning the observer perpendicular to the dominant wind direction.

Center of Gravity Analysis

The notebook's CG scatter plot (height vs. CG position) showed that rockets with the center of gravity closer to the nose cone achieved greater stability and higher altitude, a finding consistent with the Barrowman equations for model rocketry.