Comparing Projectile Angles: 30°, 45°, 60°

April 12, 2026

Problem

Compare projectile paths at 30°, 45°, and 60° with same initial velocity of 25 m/s

Explanation

Three balls are launched at the same speed but at three different angles: 30°, 45°, and 60°. Side-by-side they reveal one of the prettiest symmetries in projectile motion — and the famous result that complementary angles produce the same range.

The Physics

For launches at the same elevation:

R(θ)=v02sin(2θ)gH(θ)=v02sin2θ2gT(θ)=2v0sinθgR(\theta) = \dfrac{v_0^{2}\,\sin(2\theta)}{g} \qquad H(\theta) = \dfrac{v_0^{2}\sin^{2}\theta}{2g} \qquad T(\theta) = \dfrac{2v_0\sin\theta}{g}

Why complementary angles match: sin(2θ)=sin(180°2θ)=sin(2(90°θ))\sin(2\theta) = \sin(180° - 2\theta) = \sin(2(90° - \theta)). So θ\theta and 90°θ90° - \theta give the same sin(2θ)\sin(2\theta) — and therefore the same range. The 45° launch sits exactly at the peak of sin(2θ)\sin(2\theta), so it goes the furthest.

Step-by-Step Solution

Given: v0=25  m/sv_0 = 25\;\text{m/s}, g=9.81  m/s2g = 9.81\;\text{m/s}^{2}, three angles: 30°, 45°, 60°.

Find: RR, HH, and TT for each launch.


For θ=30°\theta = 30°:

Velocity components:

v0x=25cos30°=25×0.866021.65  m/sv_{0x} = 25\cos 30° = 25 \times 0.8660 \approx 21.65\;\text{m/s}

v0y=25sin30°=25×0.5000=12.50  m/sv_{0y} = 25\sin 30° = 25 \times 0.5000 = 12.50\;\text{m/s}

Time of flight:

T30=2(12.50)9.81=259.812.548  sT_{30} = \dfrac{2(12.50)}{9.81} = \dfrac{25}{9.81} \approx 2.548\;\text{s}

Maximum height:

H30=(12.50)22(9.81)=156.2519.627.96  mH_{30} = \dfrac{(12.50)^{2}}{2(9.81)} = \dfrac{156.25}{19.62} \approx 7.96\;\text{m}

Range:

R30=252sin60°9.81=625×0.86609.8155.16  mR_{30} = \dfrac{25^{2}\sin 60°}{9.81} = \dfrac{625 \times 0.8660}{9.81} \approx 55.16\;\text{m}


For θ=45°\theta = 45°:

v0x=v0y=25sin45°17.68  m/sv_{0x} = v_{0y} = 25\sin 45° \approx 17.68\;\text{m/s}

T45=2(17.68)9.813.604  sT_{45} = \dfrac{2(17.68)}{9.81} \approx 3.604\;\text{s}

H45=(17.68)219.62=312.519.6215.93  mH_{45} = \dfrac{(17.68)^{2}}{19.62} = \dfrac{312.5}{19.62} \approx 15.93\;\text{m}

R45=625×sin90°9.81=6259.8163.71  mR_{45} = \dfrac{625 \times \sin 90°}{9.81} = \dfrac{625}{9.81} \approx 63.71\;\text{m}


For θ=60°\theta = 60°:

v0x=25cos60°=12.50  m/sv_{0x} = 25\cos 60° = 12.50\;\text{m/s}

v0y=25sin60°21.65  m/sv_{0y} = 25\sin 60° \approx 21.65\;\text{m/s}

T60=2(21.65)9.814.414  sT_{60} = \dfrac{2(21.65)}{9.81} \approx 4.414\;\text{s}

H60=(21.65)219.62=468.7519.6223.89  mH_{60} = \dfrac{(21.65)^{2}}{19.62} = \dfrac{468.75}{19.62} \approx 23.89\;\text{m}

R60=625×sin120°9.81=625×0.86609.8155.16  mR_{60} = \dfrac{625 \times \sin 120°}{9.81} = \dfrac{625 \times 0.8660}{9.81} \approx 55.16\;\text{m}


Answer:

  • 30°: R55.16  mR \approx 55.16\;\text{m}, H7.96  mH \approx 7.96\;\text{m}, T2.55  sT \approx 2.55\;\text{s}
  • 45°: R63.71  mR \approx 63.71\;\text{m}, H15.93  mH \approx 15.93\;\text{m}, T3.60  sT \approx 3.60\;\text{s}maximum range
  • 60°: R55.16  mR \approx 55.16\;\text{m}, H23.89  mH \approx 23.89\;\text{m}, T4.41  sT \approx 4.41\;\text{s}

Notice that R30=R60R_{30} = R_{60} exactly (≈ 55.16 m) — they're complementary angles. The 60° ball reaches three times the height of the 30° ball and stays in the air 70% longer, but lands in the same spot.

Try It

  • Watch the 45° (yellow) ball reach the farthest distance — it lands about 8.5 m beyond the other two.
  • Notice the 30° (cyan) and 60° (pink) balls hit the ground at the same place — but the 60° ball arrives much later.
  • Bump the velocity to see all three paths scale uniformly. Range scales with v02v_0^{2}, so doubling the speed quadruples the range.

Interactive Visualization

Parameters

25.00
9.81
Your turn

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Comparing Projectile Angles: 30°, 45°, 60° | MathSpin