Projectile Motion Calculator
Calculate trajectory, range, time of flight, and maximum height. Solve for launch angles or speeds to hit targets, and visualize projectile paths with interactive graphs.
Calculate trajectory, range, time of flight, and maximum height. Solve for launch angles or speeds to hit targets, and visualize projectile paths with interactive graphs.
From tossing a ball to launching a rocket, projectile motion governs how objects move through the air under the influence of gravity alone. Whether you're a physics student checking homework, an educator demonstrating concepts, an athlete optimizing technique, or an engineer planning trajectories, understanding projectile motion is fundamental. Yet most people struggle with the math—separating horizontal and vertical components, applying kinematic equations correctly, and interpreting what the numbers actually mean for real-world scenarios.
Consider Alex, a high school physics student working through a problem set on projectile motion. The question: "A soccer ball is kicked at 20 m/s at a 35° angle. How far does it travel before hitting the ground?" Alex knows the formulas exist—something about v₀ cos(θ) and v₀ sin(θ)—but applying them in sequence, keeping track of which component affects which motion, and avoiding unit conversion errors is overwhelming. Using a projectile motion calculator, Alex enters the initial speed (20 m/s), angle (35°), and gravity (9.81 m/s² for Earth), and instantly sees: time of flight 2.34 seconds, horizontal range 38.3 meters, maximum height 6.72 meters. More importantly, the step-by-step breakdown shows how each value was calculated—horizontal velocity 16.38 m/s, vertical velocity 11.47 m/s—allowing Alex to verify each step, catch conceptual mistakes, and build intuition for how angle changes affect range and height.
Now consider Coach Maria, a track and field coach working with shot put athletes. She knows that optimizing the release angle is critical: too low and the shot falls short, too high and it stays airborne longer but doesn't travel as far horizontally. The theoretical "optimal angle" is 45° on level ground, but her athletes release from ~2 meters above ground level (shoulder height), which shifts the optimal angle. Using a projectile motion calculator with initial height set to 2 meters, she discovers that the optimal release angle drops to approximately 42–43°, depending on release speed. She tests this with her athletes: a 12 m/s release at 42° yields 16.8 meters range, while 45° yields only 16.5 meters—a 30 cm difference that can determine medal placement. The calculator becomes a training tool, allowing athletes to model their personal release height and speed to find their optimal technique.
This calculator helps you solve three core types of projectile motion problems: (1) Forward calculation—given initial speed, angle, and height, find range, time of flight, and maximum height. (2) Inverse calculation—given a target range and height, find the required launch angle(s) and speed. (3) Optimization—find the launch angle that maximizes range for a given speed and height. You can model scenarios on Earth, the Moon, Mars, or any custom gravity environment. You can visualize trajectories with interactive graphs showing how the projectile's path changes with angle, speed, or gravity. You can compare multiple launches side-by-side to see trade-offs between low trajectories (fast, direct) and high trajectories (slower, clears obstacles).
The stakes are surprisingly high. In physics education, projectile motion is the gateway to understanding vector decomposition, independent motion in perpendicular directions, and energy conservation—concepts that underpin all of mechanics. A student who masters projectile motion gains intuition for how forces and motion work in two dimensions, preparing them for more advanced topics like circular motion, orbital mechanics, and fluid dynamics. In sports, tiny adjustments to release angle or speed can mean the difference between a personal record and a failed attempt. A basketball player who understands the optimal arc (typically 45–52° depending on release height and distance to basket) shoots more efficiently. A golfer who knows how launch angle and spin affect carry distance and roll can select clubs and adjust swing accordingly.
Beyond education and sports, projectile motion applies to engineering (designing water fountains, planning drone flight paths, modeling ballistics for safety testing), video game physics (ensuring realistic projectile behavior in games), and even space exploration (understanding how projectiles behave under different planetary gravities). This calculator transforms abstract equations into concrete insights, helping you predict outcomes, troubleshoot errors, verify calculations, and build deep physical intuition for how objects move through space.
Projectile motion describes the motion of an object launched into the air and moving under the influence of gravity alone (ignoring air resistance). The key insight: motion in the horizontal and vertical directions is independent. Horizontal motion proceeds at constant velocity (no acceleration), while vertical motion experiences constant downward acceleration due to gravity.
The initial velocity (v₀) is the speed at which the projectile is launched, measured in meters per second (m/s) or feet per second (ft/s). The launch angle (θ) is the angle above the horizontal at which the projectile is launched, measured in degrees. Together, these determine the initial horizontal component (v₀ₓ = v₀ cos θ) and vertical component (v₀ᵧ = v₀ sin θ) of velocity. For example, launching at 20 m/s at 30° gives v₀ₓ = 20 × cos(30°) = 17.32 m/s horizontally and v₀ᵧ = 20 × sin(30°) = 10 m/s vertically.
Gravity (g) is the constant downward acceleration acting on the projectile. On Earth, g = 9.81 m/s² (or approximately 32.2 ft/s²). Gravity only affects the vertical component of motion—it does not change the horizontal velocity. The Moon has lower gravity (1.62 m/s²), resulting in longer flight times, higher maximum heights, and greater ranges for the same initial velocity and angle. Mars has intermediate gravity (3.71 m/s²), falling between Moon and Earth values.
Time of flight (T) is the total duration the projectile spends in the air, from launch until it returns to the ground (or the specified final height). For a projectile launched from ground level (h₀ = 0) and landing at ground level, the time of flight is T = (2 v₀ sin θ) / g. If the projectile is launched from a height h₀ > 0, the formula becomes more complex and is typically solved using the quadratic formula applied to the vertical position equation.
Horizontal range (R) is the total horizontal distance traveled by the projectile during its flight. Since horizontal velocity is constant (v₀ₓ = v₀ cos θ), the range is simply R = v₀ₓ × T = (v₀ cos θ) × T. For level ground launches (h₀ = 0), this simplifies to R = (v₀² sin 2θ) / g, showing that range depends on both the initial speed squared and the sine of twice the launch angle. The maximum range occurs at θ = 45° when h₀ = 0.
Maximum height (H) is the highest vertical position reached by the projectile. This occurs when the vertical velocity component becomes zero (at the peak of the trajectory). Using the kinematic equation v² = v₀² + 2aΔy, we set final vertical velocity to zero and solve for height: H = h₀ + (v₀ sin θ)² / (2g). Maximum height depends on the vertical component of initial velocity and the strength of gravity. Higher launch angles and faster speeds produce greater maximum heights, while stronger gravity reduces maximum height.
The path traced by a projectile in ideal conditions (no air resistance) is a parabola—a smooth, symmetric curve. For launches from ground level (h₀ = 0), the trajectory is symmetric: the time to reach maximum height equals the time to descend from maximum height back to ground level, and the launch angle equals the impact angle. When launching from a height (h₀ > 0), the trajectory becomes asymmetric: the projectile spends more time descending than ascending, and the impact angle is steeper than the launch angle. The parabolic shape arises from the combination of constant horizontal velocity and linearly changing vertical velocity.
Projectile motion calculations rely on separating horizontal and vertical motion into independent components, applying kinematic equations to each direction, and combining results to find range, time of flight, maximum height, and trajectory. Here's the complete mathematical framework with a worked example.
The initial velocity v₀ is decomposed into horizontal (v₀ₓ) and vertical (v₀ᵧ) components using trigonometry. The horizontal component remains constant throughout flight (no horizontal forces in ideal projectile motion), while the vertical component changes due to gravitational acceleration.
Horizontal position increases linearly with time (constant velocity). Vertical position follows a parabolic equation due to constant downward acceleration (gravity). The term ½ g t² represents the distance fallen due to gravity, which increases quadratically with time.
Scenario:
Step-by-Step Calculation:
1. Decompose velocity into components:
v₀ₓ = 20 × cos(35°) = 20 × 0.8192 = 16.38 m/s
v₀ᵧ = 20 × sin(35°) = 20 × 0.5736 = 11.47 m/s
2. Calculate time of flight (h₀ = 0):
T = (2 × 20 × sin(35°)) / 9.81
T = (2 × 20 × 0.5736) / 9.81
T = 22.94 / 9.81 = 2.34 seconds
3. Calculate horizontal range:
R = (20² × sin(2 × 35°)) / 9.81
R = (400 × sin(70°)) / 9.81
R = (400 × 0.9397) / 9.81
R = 375.88 / 9.81 = 38.3 meters
4. Calculate maximum height:
H = 0 + (20 × sin(35°))² / (2 × 9.81)
H = (11.47)² / 19.62
H = 131.56 / 19.62 = 6.71 meters
5. Verify with position equations (optional check at t = T/2 = 1.17 s):
x(1.17) = 16.38 × 1.17 = 19.16 m ≈ R/2 ✓
y(1.17) = 11.47 × 1.17 - ½ × 9.81 × (1.17)² = 13.42 - 6.71 = 6.71 m = H ✓
Result: The soccer ball stays in the air for 2.34 seconds, travels 38.3 meters horizontally, and reaches a maximum height of 6.71 meters above the ground. The trajectory is a parabola peaking halfway through the flight time and halfway through the horizontal range (for level ground launches).
Key insight: Changing the launch angle to 45° (with the same 20 m/s speed) would increase range to 40.8 meters but also increase maximum height to 10.2 meters and time of flight to 2.89 seconds. The 35° angle produces a lower, faster trajectory that's often preferred in sports where quick ball arrival matters more than clearing obstacles.
You're assigned a homework problem: "A ball is thrown horizontally at 15 m/s from a cliff 45 meters high. How far from the base of the cliff does it land?" You solve it manually, getting 45 meters horizontal range, but suspect an error. Using the calculator: initial speed 15 m/s, angle 0° (horizontal), height 45 m, gravity 9.81 m/s². Result: time of flight 3.03 seconds, range 45.5 meters. Close to your answer, but the small discrepancy reveals you used √(2h/g) ≈ 3 seconds instead of the exact 3.03 seconds. The calculator's step-by-step breakdown shows: T = √(2 × 45 / 9.81) = √9.174 = 3.03 s, then R = 15 × 3.03 = 45.5 m. You revise your solution, use more precision, and understand that rounding intermediate steps introduces cumulative error. This builds better calculation habits and prevents point loss on exams.
A shot put athlete releases the shot at 13 m/s from a height of 2.1 meters (shoulder height). They currently use a 40° release angle, achieving a 17.2-meter throw. The coach wants to optimize the angle for maximum distance. Using the calculator with 13 m/s speed, 2.1 m height, and testing angles from 35° to 45°, the results show: 35° → 17.5 m, 38° → 17.8 m, 40° → 17.7 m, 42° → 17.5 m, 45° → 16.9 m. The optimal angle is approximately 38–39°, not the intuitive 45°, because the launch height shifts the optimal angle lower. The athlete adjusts technique, practices the 38° release, and gains an extra 0.6 meters—enough to move from 4th to 2nd place in competition. The calculator becomes a training tool for modeling individual biomechanics (release speed and height vary by athlete) and finding personalized optimal angles.
A science educator demonstrates how gravity affects projectile motion by comparing the same launch (20 m/s at 45°) on Earth, Moon, and Mars. On Earth (g = 9.81 m/s²): range 40.8 m, max height 10.2 m, time 2.89 s. On the Moon (g = 1.62 m/s²): range 247 m, max height 61.7 m, time 17.5 s. On Mars (g = 3.71 m/s²): range 108 m, max height 27.0 m, time 7.64 s. Students see that weaker gravity produces dramatically longer flights—Moon projectiles travel 6× farther than on Earth—because objects fall more slowly, giving more time for horizontal travel. This builds intuition for why astronauts can "leap" much farther on the Moon and why future Mars explorers could throw equipment much greater distances. The calculator makes these comparisons instant and visual, reinforcing the relationship between g, time of flight, and range.
A medieval reenactment group is building a historically accurate trebuchet that launches projectiles at 25 m/s. They want to hit a target 55 meters away at the same height as the launch point. What angle(s) should they use? Using the calculator's inverse/target mode (or manually testing angles): the range formula R = (v₀² sin 2θ) / g gives 55 = (625 sin 2θ) / 9.81, so sin 2θ = 0.8618, meaning 2θ = 59.5° or 120.5°, giving θ = 29.75° or 60.25°. Two solutions exist: a low trajectory (29.75°, faster, 2.54 s flight) and a high trajectory (60.25°, slower, 4.44 s flight, clears obstacles). They test both and choose the low trajectory for speed and accuracy, achieving consistent hits. The calculator helps them understand that most ranges (except maximum) can be achieved with two different angles—critical knowledge for designing reliable projectile systems.
A landscape architect is designing a decorative water fountain with jets that shoot water at various angles and speeds to create an arc pattern. The tallest central jet shoots at 6 m/s at 75°, while outer jets shoot at 4 m/s at 50°. Using the calculator for the central jet: range 1.74 m, max height 1.70 m, time 1.18 s. For outer jets: range 1.57 m, max height 0.62 m, time 0.62 s. The architect confirms that the splash zone (where water lands) extends to about 1.75 meters from each jet, allowing her to plan drain placement and walkway distances to keep visitors dry. She also models different angles to create layered arcs: 80° jets for tall, narrow arcs (centerpiece), 60° for medium arcs, and 40° for wide, low arcs (perimeter). The calculator turns artistic vision into precise engineering specs, ensuring water flow, pump pressure, and aesthetics align perfectly.
A game developer is implementing projectile physics for arrows in a medieval combat game. Players complain that arrows "float" unrealistically and travel too far. The developer checks the game code: arrows are launched at 50 m/s at 30°, with gravity set to 5 m/s² (half of Earth's actual gravity). Using the calculator with Earth gravity (9.81 m/s²): range 220 m, time 5.1 s. With the game's current 5 m/s² gravity: range 433 m, time 10 s—nearly double the realistic range and flight time. The developer increases gravity to 9.81 m/s², re-tests, and players now report arrows feel "weighty" and realistic. The calculator becomes a reference tool for tuning game physics to match player expectations of realism, balancing playability (slightly exaggerated physics for fun) with believability (not too floaty).
A cinematography team uses drones for aerial shots and needs to model emergency landing trajectories if a drone loses power mid-flight. A typical drone flies at 15 m/s horizontally at 30 meters altitude. If power is lost, it will follow a projectile path (initial horizontal velocity 15 m/s, initial vertical velocity 0 m/s, height 30 m). Using the calculator: time to ground = √(2 × 30 / 9.81) = 2.47 s, horizontal distance traveled = 15 × 2.47 = 37 meters. The team establishes a safety perimeter of 50 meters around the flight path to account for wind and variability, ensuring crew and bystanders stay clear of potential landing zones. The calculator helps quantify risk and define safe operating procedures, turning "best guess" safety margins into data-driven protocols.
A physics teacher sets up a projectile launcher lab where students fire a ball at 5 m/s from a table 1 meter high and measure where it lands. Students predict the range using the calculator (5 m/s horizontal, 0° angle, 1 m height): time 0.45 s, range 2.25 m. They place a target at 2.25 m, launch the ball, and measure actual landing at 2.1 m—a 7% error. The discrepancy sparks discussion: air resistance (not modeled in ideal projectile motion), measurement error in launch speed (students used a crude spring launcher), and initial height uncertainty (ball center vs table edge). The calculator provides the ideal baseline, making real-world deviations measurable and meaningful. Students learn that models simplify reality and experimental technique matters for matching theory to practice.
Most calculators and physics problems use degrees for launch angle (0° to 90°), but some scientific calculators and programming environments default to radians (0 to π/2 ≈ 1.571). Entering 45 when the calculator expects radians (treating it as 45 radians ≈ 7.2 full rotations) produces nonsensical results. Always check the calculator's unit setting or convert: degrees to radians = degrees × π / 180, radians to degrees = radians × 180 / π. If results look wrong (e.g., negative range, impossibly large time), verify angle units first.
Earth's gravity is 9.81 m/s² (metric) or 32.2 ft/s² (imperial). Mixing units—using 9.81 when speed is in ft/s or 32.2 when speed is in m/s—produces errors by a factor of ~3.3. Always match units: if speed is m/s and height is meters, use g = 9.81 m/s². If speed is ft/s and height is feet, use g = 32.2 ft/s². Additionally, using 10 m/s² as a "round number" approximation introduces 2% error, which compounds across calculations. For homework and exams, use the exact value provided (typically 9.8 or 9.81 m/s²).
The standard projectile motion equations assume no air resistance—an ideal, simplified model. In reality, air drag reduces range, maximum height, and time of flight, especially for high-speed, low-mass, or high-surface-area projectiles (e.g., a ping pong ball or shuttlecock). A soccer ball kicked at 25 m/s might reach 50 meters with air resistance but the calculator predicts 63 meters without. Use calculator results as upper bounds: actual performance will be 5–30% lower depending on drag. For precise real-world modeling (e.g., golf, baseball, artillery), use advanced ballistics software that includes drag coefficients and wind.
The initial speed v₀ is the total magnitude of velocity, not just the horizontal or vertical part. If a problem states "horizontal velocity is 10 m/s and vertical velocity is 8 m/s at launch," the initial speed is v₀ = √(10² + 8²) = √164 = 12.8 m/s, and the angle is θ = arctan(8/10) = 38.7°. Entering 10 m/s as initial speed produces incorrect results. Conversely, if given "initial speed 15 m/s at 30°," the horizontal component is 15 cos(30°) = 13.0 m/s, not 15 m/s. Always clarify whether the problem gives total velocity (magnitude) or components (x and y).
Time to reach maximum height is half the total time of flight only for symmetric trajectories (h₀ = 0, landing at same height as launch). If launching from a height, time up ≠ time down. For example, launching from 10 meters height at 20 m/s at 60° gives time to max height 1.77 s but total time of flight 4.95 s—time descending is 3.18 s (much longer than time ascending). Students often calculate t_max = v₀ sin θ / g and assume that's total time, forgetting to solve the full quadratic for landing. Always use the complete time-of-flight formula when h₀ > 0.
In ideal projectile motion, there are no horizontal forces, so horizontal velocity v₀ₓ = v₀ cos θ remains constant throughout flight. Students sometimes apply acceleration equations to the horizontal direction (e.g., using x = ½ a t²), which is incorrect. Horizontal motion is simply x = v₀ₓ × t (constant velocity). Only the vertical direction has acceleration (gravity). This misconception often arises from mixing up equations or applying kinematic formulas without checking which direction they apply to.
The simplified range formula R = (v₀² sin 2θ) / g applies only when h₀ = 0 and landing height = 0 (level ground). When launching from a height h₀ > 0, this formula underestimates range because it ignores the extra flight time gained from the initial altitude. For height-adjusted range, first find time of flight using the quadratic formula, then calculate R = (v₀ cos θ) × T. For example, launching at 20 m/s, 45° from 5 m height: level-ground formula gives 40.8 m, but actual range with height is ~46 m (+13% error). Always check problem conditions before choosing formulas.
For level-ground launches (h₀ = 0), projectile motion is symmetric: the path up mirrors the path down, and complementary angles (e.g., 30° and 60°) produce the same range. Students sometimes think 30° and 60° produce different ranges, but both give R = (v₀² sin 60°) / g = (v₀² sin 120°) / g—since sin 60° = sin 120° = 0.866. However, 30° is a lower, faster trajectory (shorter time) while 60° is higher and slower (longer time). Recognizing these symmetries helps check work: if you calculate different ranges for complementary angles on level ground, you've made an error.
Mixing units is a common source of errors. For example, if speed is given as 72 km/h and height as 10 meters, you must convert 72 km/h to m/s: 72 km/h = 72 × 1000 / 3600 = 20 m/s. Entering 72 directly (while using g = 9.81 m/s² and height in meters) produces results off by a factor of 3.6. Similarly, mixing feet and meters (1 ft ≈ 0.305 m) causes large errors. Create a habit: list all given values with units, convert everything to a consistent unit system (SI or imperial), then calculate. Many calculators have built-in unit converters—use them before entering values.
The 45° optimal angle is true only for level ground (h₀ = 0). When launching from a height h₀ > 0, the optimal angle decreases below 45° because the projectile already has vertical "head start" from the altitude. The exact optimal angle is θ_opt = arctan(v₀ / √(v₀² + 2 g h₀)). For example, launching from 5 meters at 20 m/s: optimal angle is ~43.3°, not 45°. For very tall launches (e.g., 50 m height, 20 m/s speed), optimal angle drops to ~38°. Always account for height when optimizing angle—using 45° when h₀ > 0 leaves range on the table.
Build intuition by systematically varying one parameter at a time and observing outputs. Fix speed at 20 m/s and height at 0 m, then test angles from 15° to 75° in 5° increments. Plot or tabulate the results: you'll see range increase from 15° to 45°, then decrease from 45° to 75°, while max height increases monotonically and time of flight follows max height. Next, fix angle at 45° and vary speed from 10 to 50 m/s: range and max height increase quadratically (doubling speed quadruples range), while time increases linearly. Finally, fix speed and angle and test different gravities (1 to 10 m/s²): weaker gravity produces longer flight and greater range. These systematic explorations reveal the functional relationships between variables (quadratic vs linear dependencies, symmetric properties, optimal points) far better than solving isolated problems.
For level ground (h₀ = 0), maximum range occurs when dR/dθ = 0. Since R = (v₀² sin 2θ) / g, take the derivative: dR/dθ = (v₀² × 2 cos 2θ) / g. Setting this to zero gives cos 2θ = 0, so 2θ = 90°, thus θ = 45°. For h₀ > 0, the derivation is more complex (requires calculus and the quadratic time formula), yielding θ_opt = arctan(v₀ / √(v₀² + 2 g h₀)). Verify this with the calculator: for v₀ = 20 m/s, h₀ = 10 m, g = 9.81 m/s², the formula gives θ_opt = arctan(20 / √(400 + 196.2)) = arctan(20 / 24.42) = 39.3°. Test this in the calculator: 39° gives 53.1 m range, 39.3° gives 53.2 m, 40° gives 53.1 m, 45° gives 51.0 m—confirming 39.3° is indeed optimal. Deriving and verifying formulas deepens understanding and builds confidence in both theory and numerical tools.
For level ground, the range formula R = (v₀² sin 2θ) / g shows that range depends on sin 2θ. Since sin(180° - x) = sin(x), we have sin(2θ) = sin(180° - 2θ). Thus, angles θ and (90° - θ) produce the same sin 2θ and therefore the same range. For example, θ = 30° gives sin(60°) = 0.866, and θ = 60° gives sin(120°) = sin(60°) = 0.866—same range. Test with the calculator: 20 m/s at 30° → 35.3 m, at 60° → 35.3 m (identical range but different trajectories: 30° is low/fast, 60° is high/slow). This complementary angle property is useful for solving inverse problems (hitting a target): if one angle works, the complement also works. However, this symmetry breaks when h₀ > 0 because time of flight becomes angle-dependent in a non-symmetric way.
Projectile motion conserves total mechanical energy (ignoring air resistance). At launch: KE = ½ m v₀², PE = m g h₀, total E = ½ m v₀² + m g h₀. At maximum height: KE = ½ m v₀ₓ² (only horizontal velocity remains), PE = m g H. At impact: KE = ½ m v_impact², PE = 0 (if landing at ground level). Use the calculator to find v_impact and H, then check energy conservation. Example: 20 m/s at 45°, h₀ = 5 m. E_initial = ½ m (20)² + m (9.81)(5) = 200m + 49.05m = 249.05m. Calculator gives H = 15.2 m, v_impact = 22.1 m/s. E_max_height = ½ m (14.14)² + m (9.81)(15.2) = 100m + 149.11m ≈ 249m ✓. E_impact = ½ m (22.1)² = 244m ≈ 249m (small rounding error). This cross-verification builds confidence and reinforces the connection between kinematics and energy methods.
Some problems have multiple constraints (e.g., "hit a target 50 m away and 10 m high" or "maximize range while clearing a 5 m obstacle at 20 m distance"). The calculator can solve these via iteration: test a range of angles and speeds, filter results that meet all constraints, then optimize among valid solutions. Example: clear a 5 m wall at 20 m horizontal distance, then maximize total range. Test angles 40° to 70° at 15 m/s: record height at x = 20 m for each angle using the trajectory equation y = x tan θ - (g x²) / (2 v₀² cos² θ). Find which angles give y(20) ≥ 5 m, then among those, select the angle with maximum total range. This iterative, constraint-filtering approach is how engineers solve real-world trajectory design problems, and the calculator makes it tractable without custom code.
Use the calculator's ideal predictions as a baseline for experiments or real-world measurements. Example: kick a soccer ball at measured 22 m/s at 40° and measure landing at 42 meters. The calculator predicts 48.1 meters (ideal, no drag). The shortfall (48.1 - 42 = 6.1 m, ~13% reduction) quantifies air resistance. Repeat for different speeds and angles: higher speeds experience more drag (quadratic with velocity), while higher angles (more vertical motion, more time in air) also lose more energy to drag. By comparing ideal vs actual, you can estimate drag coefficients, validate physics models, and develop correction factors. This is how sports scientists optimize equipment (golf ball dimples, baseball seams) to minimize drag and maximize range.
Most introductory problems assume landing at ground level (y_final = 0), but real scenarios often involve landing below or above launch height (e.g., throwing downhill, shooting uphill). Modify the time-of-flight equation to solve for when y(T) = y_final instead of y(T) = 0. Example: launch from a 30 m cliff at 15 m/s at 20° toward water 30 m below (y_final = -30 m). Set -30 = 30 + (15 sin 20°)T - ½ (9.81) T² and solve the quadratic: T ≈ 3.6 s, giving range R = (15 cos 20°) × 3.6 ≈ 50.8 m. Uphill shots (y_final > 0) reduce range and flight time, while downhill (y_final < 0) increase both. Use the calculator's custom final-height option (if available) or manually solve the quadratic to explore these scenarios, which are common in sports (golf tee shot to elevated green, ski jump landing).
The trajectory equation y(x) = x tan θ - (g x²) / (2 v₀² cos² θ) describes the projectile's height as a function of horizontal distance. Use this to find the maximum safe clearance at any horizontal position. Example: launching at 20 m/s at 50° to clear a building 30 m away and 12 m tall. Calculate y(30): y = 30 tan(50°) - (9.81 × 30²) / (2 × 20² × cos²(50°)) = 30(1.192) - (8829) / (2 × 400 × 0.413) = 35.76 - 26.73 = 9.03 m. The projectile is at 9.03 m height when x = 30 m, clearing the 12 m building is impossible with this launch—it passes below. Increase angle to 60°: y(30) = 30(1.732) - 26.73 / cos²(60°) = 51.96 - 26.73/0.25 = 51.96 - 106.92 (this formula breaks for large angles; recalculate properly). Use the calculator or plot y(x) to find safe trajectories that clear obstacles at all points along the path.
For long-range projectiles (e.g., artillery, intercontinental ballistics), Earth's rotation introduces the Coriolis effect, deflecting the trajectory sideways. This is beyond standard projectile motion but can be modeled by adding a small lateral acceleration term proportional to velocity and latitude. For a rough estimate, the Coriolis deflection is approximately d_Coriolis ≈ (ω × v × T²) / 2, where ω is Earth's rotation rate (~7.3 × 10⁻⁵ rad/s), v is velocity, and T is flight time. For a 5-second flight at 30° latitude, this deflection is ~0.5 meters—negligible for sports but critical for long-range military or space applications. Use the calculator's standard output (range, time) as inputs to Coriolis correction formulas for high-precision trajectory planning.
Projectile motion is a special case of orbital mechanics: when initial speed is low, the projectile follows a parabolic arc and hits the ground. As speed increases, the curvature of Earth becomes relevant—the projectile "falls" around the planet instead of hitting it. The orbital velocity for low Earth orbit is ~7.8 km/s (7800 m/s). Use the calculator to explore this transition: launch at 45° from 100 km altitude (ignoring atmosphere) with increasing speeds: 500 m/s → falls to Earth in minutes, 2000 m/s → travels farther but still falls, 7800 m/s → orbits Earth indefinitely. The transition from ballistic trajectory to orbit happens when horizontal velocity matches the rate at which Earth curves away. This conceptual bridge connects introductory mechanics (projectile motion) to advanced topics (spacecraft trajectories, orbital insertion, escape velocity).
The Projectile Motion Calculator provides several key outputs to help you understand the trajectory and motion characteristics of the projectile:
Total duration the projectile spends in the air, from launch until it returns to the final height (typically ground level). Measured in seconds. Longer times of flight occur with higher launch angles (more vertical motion), higher initial speeds, weaker gravity, or greater launch heights. For level-ground launches, time to reach maximum height is exactly half the total time of flight due to trajectory symmetry.
Total horizontal distance traveled by the projectile during its flight, measured from the launch point to the landing point. Measured in meters or feet. Range increases with initial speed (quadratically—doubling speed quadruples range), optimal launch angle (45° for level ground, slightly less when launching from height), and weaker gravity. Complementary angles (e.g., 30° and 60°) produce the same range on level ground but different trajectory shapes.
The highest vertical position reached by the projectile above the launch point, measured in meters or feet. Maximum height depends on the vertical component of initial velocity (v₀ sin θ) and gravity. Higher launch angles and faster speeds produce greater maximum heights. At maximum height, the vertical velocity component is zero (momentarily), while horizontal velocity remains constant. The projectile spends equal time ascending to and descending from maximum height (for level ground launches).
The velocity at which the projectile hits the ground, broken into horizontal (vₓ) and vertical (vᵧ) components, along with the total magnitude (v_impact). The horizontal component equals the initial horizontal velocity (v₀ cos θ) because there's no horizontal acceleration. The vertical component at impact typically exceeds the initial vertical component because gravity accelerates the projectile downward throughout the flight. For symmetric trajectories (level ground), the impact speed equals the launch speed, but the angle is opposite (downward instead of upward).
Many calculators display an interactive graph showing the parabolic path of the projectile, with horizontal distance on the x-axis and vertical height on the y-axis. The graph helps visualize how angle and speed affect trajectory shape: low angles produce wide, flat parabolas (max range, low height), high angles produce tall, narrow parabolas (max height, less range), and 45° balances both for maximum range. The apex of the parabola occurs at horizontal distance R/2 (halfway through the flight) for level-ground launches. Use the graph to identify clearance points over obstacles or to compare multiple launch scenarios side-by-side.
If calculator results differ significantly from measured data or intuition, check: (1) Unit consistency—ensure all inputs use the same unit system (metric or imperial). (2) Angle units—verify degrees vs radians. (3) Air resistance—real-world drag can reduce range by 10–30% for typical sports projectiles; calculator assumes ideal conditions. (4) Initial height—failing to account for launch height (even 1–2 meters) can shift results noticeably. (5) Measurement error—actual launch speed and angle may differ from intended values; small errors in angle (±5°) can change range by 10–20%. (6) Gravity setting—ensure you're using the correct g value for your planet/environment. Use the calculator as a baseline, then investigate discrepancies to identify real-world factors or experimental errors.
• No Air Resistance (Vacuum Trajectory): This calculator assumes projectile motion in a vacuum with no drag forces. Real projectiles experience air resistance that depends on velocity squared, reducing range by 10-50% for typical sports balls and significantly more for high-speed or lightweight objects.
• Constant Gravitational Acceleration: Calculations use a uniform gravitational field (g = 9.8 m/s² by default). For very high trajectories or long-range ballistics, variations in gravity with altitude and the Earth's rotation (Coriolis effect) become significant factors.
• Point Mass Approximation: The projectile is treated as a point particle with no spin, rotation, or aerodynamic lift effects. Real projectiles like golf balls, baseballs, and soccer balls experience Magnus effect and other spin-dependent forces that substantially alter their trajectories.
• Flat Earth Over Short Ranges: The calculator assumes a flat, non-rotating Earth. For ballistic missiles, artillery at long range, or any trajectory exceeding several kilometers, Earth's curvature and rotation must be considered for accurate predictions.
Important Note: This calculator is strictly for educational and informational purposes only. It demonstrates idealized projectile motion physics for learning. Real-world applications in sports science, ballistics, or engineering require drag coefficients, wind analysis, and computational methods beyond the scope of this educational tool.
The formulas and principles used in this calculator are based on established physics principles from authoritative sources:
Note: This calculator implements standard physics formulas for educational purposes assuming no air resistance. For applications requiring high precision or air resistance effects, consult ballistics references and engineering standards.
Common questions about projectile motion calculations, launch angles, gravity settings, trajectory analysis, and real-world applications.
No—this calculator models ideal projectile motion, assuming no air resistance. Real projectiles experience drag that reduces range, maximum height, and time of flight by 5–30% depending on speed, mass, surface area, and shape. For example, a soccer ball at 25 m/s loses ~15% of its ideal range due to drag, while a ping pong ball loses ~40%. Use this calculator's results as upper-bound estimates for real-world scenarios. For precision applications requiring drag modeling (golf, artillery, aerospace), use specialized ballistics software that includes drag coefficients, Reynolds numbers, and wind effects.
Most calculators accept meters per second (m/s) for speed, meters (m) for height and distance, and degrees (°) for launch angle, with gravity defaulting to 9.81 m/s² (Earth, metric). Some also support imperial units: feet per second (ft/s) for speed, feet (ft) for distance, and 32.2 ft/s² for gravity. Always ensure all inputs use the same unit system—mixing metric and imperial produces errors by factors of ~3.3×. For speed conversions: 1 m/s = 3.28 ft/s = 3.6 km/h = 2.24 mph. Angles are typically in degrees (0–90°), not radians; if using radians, 45° = π/4 ≈ 0.785 radians.
For level-ground launches (h₀ = 0), the range formula R = (v₀² sin 2θ) / g is maximized when sin 2θ = 1, which occurs at 2θ = 90°, giving θ = 45°. At 45°, the horizontal and vertical velocity components are equal (v₀ cos 45° = v₀ sin 45° ≈ 0.707 v₀), balancing horizontal distance traveled with vertical time in air. Angles below 45° have more horizontal speed but less flight time (fall faster), while angles above 45° have more flight time but less horizontal speed—45° optimizes the product. However, this is only true for level ground; when launching from a height h₀ > 0, the optimal angle decreases to ~38–43° depending on height and speed.
Yes—entering 90° models a purely vertical launch. The projectile rises to maximum height H = h₀ + v₀² / (2g), then falls back down. Time of flight is T = 2v₀ / g (for h₀ = 0), and horizontal range is R = 0 meters (no horizontal component). For example, launching at 20 m/s straight up on Earth: max height 20.4 meters, time of flight 4.08 seconds, range 0 meters. This is useful for modeling objects dropped from height (0° horizontal), thrown straight up (90°), or rockets ascending vertically before trajectory correction. At 90°, all initial velocity is vertical (v₀ₓ = 0, v₀ᵧ = v₀).
Lower gravity produces longer flight times, greater maximum heights, and longer ranges for the same initial speed and angle. Moon (g = 1.62 m/s², ~1/6 Earth): a 20 m/s launch at 45° travels 247 meters vs 40.8 m on Earth—over 6× farther—and reaches 61.7 m max height vs 10.2 m on Earth. Mars (g = 3.71 m/s², ~1/3 Earth): same launch travels 108 m and reaches 27.0 m height. Weaker gravity slows the downward acceleration, giving the projectile more time to travel horizontally. This is why astronauts on the Moon can 'leap' much farther and why future Mars explorers could throw objects 3× farther than on Earth. Use the gravity dropdown or custom input to explore different planetary environments.
Launching from a height h₀ > 0 increases both range and time of flight compared to ground-level launches, because the projectile has more time to travel horizontally before hitting the ground. The trajectory becomes asymmetric: time ascending to max height is less than time descending to ground level. For example, launching at 20 m/s at 45° from ground level (h₀ = 0) gives 40.8 m range and 2.89 s flight time. From h₀ = 5 m, range increases to ~46 m and time to ~3.25 s. The optimal angle for maximum range also shifts lower: from 45° at h₀ = 0 to ~43° at h₀ = 5 m to ~38° at h₀ = 20 m. Always include launch height for realistic modeling of throws from platforms, cliffs, or shoulder height.
For most ranges (except maximum range at 45°), two complementary angles produce the same horizontal distance. This occurs because the range formula R = (v₀² sin 2θ) / g depends on sin 2θ, and sin(2θ) = sin(180° - 2θ). For example, sin(60°) = sin(120°), so angles 30° and 60° yield identical ranges—both equal ~35.3 m for 20 m/s launches on level ground. However, the trajectories differ: 30° is a low, fast trajectory (shorter flight time, lower max height), while 60° is a high, slow trajectory (longer flight time, higher max height). In practice, low angles are preferred for speed and precision (sports, direct hits), while high angles clear obstacles (lob shots, mortar fire). This symmetry only holds for level ground (h₀ = 0); launching from height breaks the complementary angle property.
For level ground (h₀ = 0), use the range formula R = (v₀² sin 2θ) / g and solve for θ: sin 2θ = R g / v₀², so 2θ = arcsin(R g / v₀²), giving θ = ½ arcsin(R g / v₀²). This yields two solutions (complementary angles) if R < R_max. Example: hit a target 50 m away with 25 m/s speed on Earth. sin 2θ = (50 × 9.81) / 625 = 0.785, so 2θ = 51.7° or 128.3°, giving θ = 25.9° or 64.2°. Both angles hit the target—choose low angle (25.9°) for faster arrival or high angle (64.2°) to clear obstacles. If arcsin returns an error or sin 2θ > 1, the target is beyond maximum range—increase speed or accept that it's unreachable. For h₀ > 0, use inverse/target mode in the calculator or solve numerically.
Yes—most calculators offer presets for Earth (9.81 m/s²), Moon (1.62 m/s²), Mars (3.71 m/s²), and a custom gravity input for any value. Use custom gravity to model: other celestial bodies (Jupiter 24.79 m/s², Titan 1.35 m/s², Pluto 0.62 m/s²), hypothetical scenarios (half Earth gravity for sci-fi worldbuilding), free fall in fluids (reduced effective gravity due to buoyancy), or laboratory experiments (inclined plane simulations where effective g = g sin α). Enter gravity in the same units as your other inputs: if using m/s for speed and meters for distance, use m/s² for gravity. Testing different gravities builds intuition for how g scales all outcomes proportionally—doubling g halves range and max height.
Discrepancies between calculator (ideal) and real-world results arise from: (1) Air resistance—drag reduces range/height by 10–30%; high-speed or light projectiles lose more. (2) Measurement errors—launch speed and angle are hard to measure precisely; ±5° angle error changes range by 10–20%. (3) Spin effects (Magnus force)—spinning balls (soccer, golf, baseball) curve sideways and up/down beyond ideal parabolic motion. (4) Launch height uncertainty—failing to account for release height (even 1–2 m) shifts results. (5) Wind—headwind/tailwind and crosswinds change range and trajectory. (6) Surface effects—ball bounce, rolling, or sliding after landing affects total distance. Use calculator predictions as baselines, then investigate differences to identify real-world factors. For precision applications, use advanced ballistics models with drag coefficients (Cd), air density (ρ), and cross-sectional area (A).
The trajectory graph plots height (y-axis) vs. horizontal distance (x-axis), showing the parabolic path. Use it to visualize: (1) Maximum height location—the apex occurs at horizontal distance R/2 (halfway through flight) for level ground. (2) Trajectory shape—low angles produce wide, flat parabolas, high angles produce tall, narrow parabolas. (3) Obstacle clearance—overlay the obstacle position on the graph to see if the trajectory passes above. For example, to clear a 5 m wall at 20 m distance, find the projectile's height at x = 20 m using y = x tan θ - (g x²) / (2 v₀² cos² θ). If y(20) > 5 m, it clears; if y(20) < 5 m, it hits. Test different angles to find the minimum that clears, then add a safety margin. Many calculators let you add obstacle markers directly to the graph for visual confirmation.
Time to maximum height (t_max) is when the projectile reaches its peak altitude and vertical velocity becomes zero: t_max = v₀ sin θ / g. Total time of flight (T) is when the projectile returns to the final height (usually ground level). For symmetric trajectories (level ground, h₀ = 0), t_max = T / 2—time up equals time down. For example, 20 m/s at 60° gives t_max = 1.77 s and T = 3.54 s. For asymmetric trajectories (h₀ > 0), time descending exceeds time ascending because the projectile falls farther (from max height back to ground level, not just back to launch height). Example: same 20 m/s at 60° from h₀ = 10 m gives t_max = 1.77 s (unchanged—gravity doesn't care about start height) but T = 4.95 s (much longer descent). Always calculate T using the full quadratic formula when h₀ > 0, not simply 2 × t_max.
Yes, with caveats. The calculator models ideal projectile motion, which approximates real sports projectiles but ignores: (1) Air resistance—significant for high-speed balls (golf 30–50% range loss, soccer 15–25%, basketball 5–10%). (2) Spin effects—backspin creates lift (golf ball carries farther), topspin creates downforce (tennis ball drops faster), sidespin causes lateral curve (soccer bend). (3) Bounce and roll—golf ball roll after landing adds 10–30% to carry distance, not modeled here. Use the calculator for: initial estimates (basketball free throw angle, soccer goal kick range), optimizing launch parameters (compare 40° vs 45° release for shot put), understanding trade-offs (higher angle clears defenders but takes longer to arrive). For precision tuning (golf club fitting, baseball pitch design), use sport-specific ballistics software with drag, spin, and surface models.
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