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Full Projectile Motion Experimental Lab

A full-workflow projectile motion investigation. Choose an investigation, state your hypothesis, identify the independent and dependent variables, collect replicated trials, fit a regression line, and analyze residuals and percent error.

Choose an Investigation

Investigation A. Optimal Angle for Maximum Range

How does launch angle affect the horizontal range of a projectile, and which angle maximizes it?

Independent Variable

Launch angle θ (vary from 15° to 75° in 5° steps)

Dependent Variable

Range R (averaged from 3 measurement replicates)

Controlled Variables
  • Initial speed v (constant)
  • Local gravity g (constant)
  • Launch height h₀ (0 m, ground level)
Hypothesis Prompt

Predict which launch angle gives the longest range when launching from ground level. Will the range vs angle curve be symmetric? State a clear, testable hypothesis.

Expected Result

Range peaks at θ = 45° and the curve is symmetric about 45°. Trials at complementary angles (e.g. 30° and 60°) should produce nearly identical ranges within measurement scatter.

Procedure
  1. Fix speed and height. Record trials at 15°, 25°, 35°, 45°, 55°, 65°, 75°
  2. Plot range R vs launch angle θ
  3. Identify the angle that produced the maximum measured range
  4. Compare the data-derived optimal angle to the theoretical value of 45°
  5. Check whether complementary-angle pairs gave similar ranges

Setup

m/s
°
m
m/s²
m/s²

Each "Record Trial" simulates 3 measurements of the landing point with realistic ±0.15 m scatter. The recorded R is the average of those three replicates.

Trajectory Preview

0.011.222.433.644.90.05.911.7H = 10.19 mR = 40.77 mv = 20.0 m/s, θ = 45°horizontal distance (m)height (m)

Range R (m) vs Launch angle θ (°)

-0.050.230.500.781.05-0.100.200.500.801.10Launch angle θ (°)Range R (m)

Record at least 2 trials (or load sample data) to see the regression line.

Regression & Error Analysis

Record at least 2 trials to compute the regression. For a defensible fit you should collect 6 or more trials across the full range of the IV.

Data Table

(0 rows)
#TrialSpeed v(m/s)Angle θ(°)Launch height h₀(m)Range R (avg of 3)(m)Range std dev(m)(m²/s²)Theoretical R(m)
0 / 500
0 / 500
0 / 500

Reference Guide

Investigation Workflow

A scientific investigation needs more than a single measurement. It needs a hypothesis, a clear independent and dependent variable, repeated trials, a fit line, and an honest error analysis.

  1. State a testable hypothesis
  2. Identify IV, DV, and controlled variables
  3. Record at least 6 replicated trials across the range of the IV
  4. Fit a regression line and inspect residuals
  5. Quote a final value with uncertainty and percent error

Kinematic Equations

Horizontal and vertical motion are independent. With launch speed v and angle θ:

x(t)=vcosθtx(t) = v\cos\theta \cdot t
y(t)=h0+vsinθt12gt2y(t) = h_{0} + v\sin\theta \cdot t - \tfrac{1}{2} g t^{2}

The landing point is where y returns to 0. Solving the quadratic in t and substituting back into x gives the full range.

Range Formula

For a ground-launched projectile (h₀ = 0), the range simplifies to:

R=v2sin(2θ)gR = \frac{v^{2}\sin(2\theta)}{g}

Range is maximized at θ = 45° since sin(2θ) is maximum there. Complementary angles (e.g. 30° and 60°) give equal ranges. At 45° the formula reduces to R = v²/g, so the slope of R vs v² equals 1/g and gives an experimental derivation of gravity.

gexp=1slope of R vs v2g_{\text{exp}} = \frac{1}{\text{slope of } R \text{ vs } v^{2}}

Error Analysis

Quote the derived value with both uncertainty and percent error:

%error=gexpgacceptedgaccepted×100%\%\text{error} = \frac{|g_{\text{exp}} - g_{\text{accepted}}|}{g_{\text{accepted}}} \times 100\%

Slope uncertainty propagates to g via the relative-error rule δg/g = δslope/slope. Inspect residuals for systematic patterns. Curvature indicates that a linear fit is inappropriate (e.g. range vs angle, which is sinusoidal, not linear).

When launching from a raised platform, the simple R = v²sin(2θ)/g formula breaks down. The full range formula includes a square-root correction from the quadratic time-of-flight equation.

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