Connect projectile components through one clock
With uniform gravity and negligible air resistance, horizontal acceleration is zero while vertical acceleration is −g for an upward-positive axis. This separates the component equations: x=vₓ₀t and y=vᵧ₀t−0.5gt² for an origin at launch. The components share one elapsed time; they are not two separate trips.
Learning outcome: Hold upward velocity at 8 m/s and compare horizontal components 2,4 and 8 m/s. Then hold the horizontal component fixed and vary the vertical component. Use ratios to test the range, flight-time and height equations. State the condition needed for the return-time formula.
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Use signed quantities, algebraic substitution, graph slopes and areas. State the system, coordinate axes and units before calculating.
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For vₓ₀=6 m/s and vᵧ₀=8 m/s, T=1.6 s, range=9.6 m, apex time=0.8 s and height=3.2 m. At the apex velocity is (6,0) m/s, not zero. A second launch with horizontal component 3 m/s has half the range but the same vertical history.
Open the experimentPredict
If horizontal velocity doubles while upward velocity is fixed, which outputs double and which remain unchanged?
Experiment
Hold upward velocity at 8 m/s and compare horizontal components 2,4 and 8 m/s. Then hold the horizontal component fixed and vary the vertical component. Use ratios to test the range, flight-time and height equations. State the condition needed for the return-time formula.
Separate projectile components
Worked teaching model · synthetic values · Point projectile launched at y=0 and returning to y=0; g=10 m/s² is an assigned rounded teaching value. Uniform gravity, no drag, no collision or launch mechanism. Horizontal and vertical components are independently adjustable.
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Axes rescale with settings; compare numerical values, not screen angles or apparent lengths. Solid/points show the selected model relationship or observations; the dashed comparison is explained below.
| Quantity | Value | Unit |
|---|---|---|
| Return time | 1.6 | s |
| Apex time | 0.8 | s |
| Maximum height | 3.2 | m |
| Ground horizontal displacement | 9.6 | m |
| Observer horizontal displacement | 9.6 | m |
| Horizontal velocity in displayed frame | 6 | m/s |
| Vertical velocity at return | -8 | m/s |
Accessible plot coordinates
| horizontal position (m) | height (m) |
|---|---|
| 0 | 0 |
| 0.48 | 0.608 |
| 0.96 | 1.152 |
| 1.44 | 1.632 |
| 1.92 | 2.048 |
| 2.4 | 2.4 |
| 2.88 | 2.688 |
| 3.36 | 2.912 |
| 3.84 | 3.072 |
| 4.32 | 3.168 |
| 4.8 | 3.2 |
| 5.28 | 3.168 |
| 5.76 | 3.072 |
| 6.24 | 2.912 |
| 6.72 | 2.688 |
| 7.2 | 2.4 |
| 7.68 | 2.048 |
| 8.16 | 1.632 |
| 8.64 | 1.152 |
| 9.12 | 0.608 |
| 9.6 | 0 |
Changing horizontal velocity alone changes range, not flight time or maximum height.
Solve y=t(vy−gt/2)=0: the nonzero return time is 2vy/g. The projectile has zero vertical velocity at the apex but retains its horizontal velocity. Equal launch and landing height is essential for this time formula.
Changing horizontal velocity alone changes range, not flight time or maximum height.
Solve y=t(vy−gt/2)=0: the nonzero return time is 2vy/g. The projectile has zero vertical velocity at the apex but retains its horizontal velocity. Equal launch and landing height is essential for this time formula.
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How would you change the solution if the projectile landed 1 m above its launch height? Which component determines candidate landing times?
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