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Animated projectile arc with adjustable angle and speed. Shows parabolic trajectory and range marker.

Variables

SymbolNameSIDimensionRange
RRRangeoutput
Horizontal distance traveled by the projectile
mL0 – 5000
vvLaunch Speed
Initial speed of the projectile
m/sLT⁻¹1 – 200
θθLaunch Angle
Angle of launch above horizontal (in degrees)
°dimensionless0 – 90
ggGravitational Acceleration
Acceleration due to gravity at Earth's surface
m/s²LT⁻²9.8 – 9.8

Deep dive

Derivation
Split initial velocity into vₓ = v·cosθ and vᵧ = v·sinθ. Time of flight: T = 2v·sinθ/g. Range: R = vₓ·T = v·cosθ · 2v·sinθ/g = v²·sin(2θ)/g.
Experimental verification
Ballistic range tables, artillery firing data, and high-speed camera trajectory tracking.
Common misconceptions
  • Air resistance makes optimal angle less than 45° in practice
  • Complementary angles (30° and 60°) give equal range but different flight times
  • The formula assumes flat ground — uphill/downhill changes the optimal angle
Real-world applications
  • Sports trajectory optimization
  • Artillery and ballistics
  • Sprinkler coverage design
  • Long jump technique

Worked examples

Optimal soccer kick

Given:
v:
25
theta:
45
g:
9.8
Find: R
Solution

R = v²sin(2×45°)/g = 625×1/9.8 = 63.8 m

Complementary angles give equal range

Given:
v:
20
theta_1:
30
theta_2:
60
g:
9.8
Find: R for both angles
Solution

Both give R = 400×sin(60°)/9.8 = 400×0.866/9.8 = 35.3 m

Scenarios

What if…
  • scenario:
    What if on the Moon (g = 1.62)?
    answer:
    Range increases by factor 9.8/1.62 = 6.05×. A 63.8 m kick becomes 386 m on the Moon.
  • scenario:
    What if air resistance is included?
    answer:
    Optimal angle drops below 45° (typically 30°–40° depending on drag). Range decreases significantly at high speeds.
  • scenario:
    What if launched from a cliff (height h)?
    answer:
    The formula changes: R = (v²/2g)[sin(2θ) + √(sin²(2θ) + 8gh/v²·cos²θ)]. Higher launch point always increases range.
Limiting cases
  • condition:
    θ = 0° or 90°
    result:
    R = 0
    explanation:
    Horizontal launch has no hang time; vertical launch has no horizontal component.
  • condition:
    θ = 45°
    result:
    R = v²/g (maximum)
    explanation:
    sin(90°) = 1 gives the maximum range.
  • condition:
    g → 0
    result:
    R → ∞
    explanation:
    Without gravity, the projectile travels in a straight line forever.

Context

Galileo Galilei · 1638

Derived in Discorsi e dimostrazioni matematiche, where Galileo analyzed parabolic trajectories of cannonballs.

Hook

A soccer player kicks at 25 m/s. At what angle does the ball travel the farthest?

R = v²sin(2θ)/g is maximized when sin(2θ) = 1, i.e., θ = 45°. At 25 m/s: R = 625/9.8 ≈ 63.8 m.

Dimensions:
lhs:
R → [L]
rhs:
v²·sin(2θ)/g → [LT⁻¹]²/[LT⁻²] = [L²T⁻²]/[LT⁻²] = [L]
check:
Both sides are [L] = meters. sin(2θ) is dimensionless. ✓
Validity: Valid for flat ground, no air resistance, uniform g = 9.8 m/s², and non-relativistic launch speeds.

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