Vertical Jump Calculator

Vertical Jump Calculator finds jump height from max jump reach − standing reach, then estimates hang time, takeoff velocity, peak power, average power, and mechanical work.

Vertical Jump Distance
24.00 inches
Difference between max jump reach and standing reach.
Flight Mechanics
0.71 Seconds Hang Time
Takeoff Velocity 3.46 m/s
Jump Height 0.61 m
Total time spent airborne from takeoff to landing, determined strictly by gravitational acceleration.
Peak Power Output
5,343.86 Watts Peak Power
Relative Power 65.45 W/kg
Peak-to-Avg Ratio 3.86x
Estimated peak anaerobic power from the Sayers equation.
Average Power Output
1,383.82 Watts Average Power
Relative Avg 16.95 W/kg
Takeoff Impulse 282.32 N·s
Estimated average mechanical power from jump height and body mass using the Lewis formula.
Mechanical Work Done
488.09 Joules Mechanical Work
Relative Work 5.98 J/kg
Body-Weight Force 800.68 N
Estimated mechanical work against gravity at the jump apex.
Biomechanical Context
Vertical jump depends on rapid force production at takeoff. Peak power is estimated with the Sayers equation, average power with the Lewis formula, and hang time from takeoff velocity and gravity.

Biomechanics Behind Jump Height

A vertical jump test remains one of the most accessible field assessments of lower-body explosive power, and a Vertical Jump Calculator translates the simple difference between standing reach and maximum jump reach into a full biomechanical profile.

What begins as a single displacement measurement unlocks flight time, takeoff velocity, peak and average power output, mechanical work, and impulse—all derived from well-established physical laws and validated regression equations. Understanding each derived metric clarifies what the raw jump height actually means for athletic performance.

What a Vertical Jump Calculator Estimates

A vertical jump assessment yields far more than a height number. The following kinetic and kinematic quantities emerge directly from the reach difference, body mass, and gravitational acceleration.

Jump Displacement – The net vertical rise of the body’s centre of mass, computed as maximum jump reach minus standing reach. This is the primary output expressed in inches or centimetres.

Flight Time – Total duration spent airborne from the instant of toe-off to ground contact. Because the ascent and descent phases are symmetrical under constant gravity, flight time is determined exclusively by takeoff velocity.

Takeoff Velocity – The instantaneous vertical speed of the centre of mass at the moment the feet leave the ground. It governs both height and hang time.

Peak Power – The highest instantaneous rate of mechanical work during the propulsive phase, estimated via the Sayers equation from jump height in centimetres and body mass in kilograms.

Average Power – Mean mechanical power output over the entire jump, derived from the Lewis formula, which treats the jump as a single work pulse against gravity.

Mechanical Work – The work done against gravity to elevate the body’s mass to the apex, equal to the gain in gravitational potential energy.

Takeoff Impulse – The product of net force and the time over which it acts during push-off, equal to the change in momentum from rest to takeoff velocity.

Kinematic Relationships: Height, Velocity, and Hang Time

Three kinematic equations connect the core flight variables. All assume negligible air resistance and constant gravitational acceleration (g = 9.80665 m/s²).

Takeoff velocity (v) from jump height (h):
v = √(2 × g × h)

Hang time (t) from takeoff velocity:
t = (2 × v) / g

Height expressed in terms of flight time:
h = (g × t²) / 8

A person with a 24-inch (0.6096 m) vertical jump has the following flight profile.

Convert inches to metres: h = 24 × 0.0254 = 0.6096 m

Compute takeoff velocity:
v = √(2 × 9.80665 × 0.6096) = √11.96 ≈ 3.46 m/s

Compute hang time:
t = (2 × 3.46) / 9.80665 ≈ 0.71 s

Apex time (half of hang time) equals 0.35 s.

The velocity required to leave the ground scales with the square root of jump height. Doubling the jump height from 12 to 24 inches raises takeoff velocity by a factor of √2, from about 2.45 m/s to 3.46 m/s, and hang time increases proportionally.

Peak Power: The Sayers Equation

Direct power measurement during a vertical jump requires a force plate and motion capture. For field use, the Sayers equation provides a validated estimate of peak anaerobic power from easily obtained variables.

Sayers peak power (watts):
PP = (60.7 × jump height in cm) + (45.3 × body mass in kg) − 2055

This equation was developed on a mixed-gender sample of countermovement jumps and correlates strongly (r = 0.91) with laboratory-derived peak power. The regression coefficients capture the interplay between displacement and body mass.

Worked example for an athlete weighing 180 lb (81.65 kg) with a 24-inch (60.96 cm) jump:

Convert body mass: 180 × 0.453592 = 81.65 kg
Convert jump height: 24 × 2.54 = 60.96 cm

PP = (60.7 × 60.96) + (45.3 × 81.65) − 2055
PP = 3700.3 + 3698.7 − 2055
PP = 5344.0 watts

Relative peak power = 5344.0 / 81.65 = 65.45 W/kg

A peak power value below zero for extremely light individuals or very small jumps is clamped to zero, indicating the equation’s lower boundary.

Average Power: The Lewis Formula

While peak power captures an instantaneous effort, average power reflects sustained energy delivery during the jump. The Lewis formula models the body as a projectile and computes average mechanical power from jump height and body mass.

Lewis average power (watts):
AP = √4.9 × body mass (kg) × g × √jump height (m)

Using the same athlete:

AP = 2.2136 × 81.65 × 9.80665 × √0.6096
AP = 2.2136 × 81.65 × 9.80665 × 0.7807
AP = 2.2136 × 624.9
AP = 1383.8 watts

Relative average power = 1383.8 / 81.65 = 16.95 W/kg

The ratio between peak and average power (3.86x) indicates how pulsed the effort is. A higher ratio suggests a more explosive, rate-dependent jump profile.

Mechanical Work and Impulse

Work done against gravity equals the gain in potential energy.

Work (joules) = mass (kg) × g × jump height (m)

For the example: 81.65 × 9.80665 × 0.6096 = 488.1 J
Relative work = 5.98 J/kg

Takeoff impulse reflects the momentum imparted to the body.

Impulse (N·s) = mass (kg) × takeoff velocity (m/s)

Impulse = 81.65 × 3.46 = 282.3 N·s

Both quantities scale linearly with body mass and with jump height. Comparing relative work (J/kg) across athletes removes body mass and focuses on the quality of the jump displacement itself.

Performance Reference Ranges

Normative data for countermovement vertical jump height provides context for field-based assessments. The values below represent typical ranges for adults without sport-specific filtering.

CategoryMen (inches)Women (inches)
Excellent> 28> 24
Good24–2820–24
Average20–2416–20
Below Average< 20< 16

Elite volleyball and basketball athletes frequently exceed 30 inches, while high-level track sprinters and weightlifters also demonstrate exceptional vertical jump capacity. These norms assume a countermovement jump with arm swing; strict no-arm-swing protocols reduce height by 10–15%.

Factors Governing Vertical Jump Performance

Multiple physiological and biomechanical factors determine vertical jump height, and a single reach measurement cannot isolate each. However, understanding these contributors allows better interpretation of the metrics a vertical jump assessment provides.

Rate of Force Development (RFD) – The slope of the force-time curve during the initial push-off phase strongly influences takeoff velocity. Athletes with higher RFD generate more impulse in the limited time available before the feet leave the ground.

Stretch-Shortening Cycle – A countermovement that rapidly transitions from eccentric to concentric action stores elastic energy in tendons and triggers the myotatic stretch reflex, augmenting jump height by 10–20% compared to a purely concentric squat jump.

Body Composition – Higher body fat percentage adds non-contributing mass that reduces acceleration for a given force output. Relative power (W/kg) adjusts for total body mass, though lean mass is the relevant contractile tissue.

Anthropometry – Limb length, tendon insertion points, and muscle architecture affect leverage and force transmission. Two individuals with identical power output may achieve different jump heights due to structural differences.

Arm Swing Contribution – An upward arm swing contributes approximately 10–15% additional jump height through increased impulse and centre-of-mass elevation at takeoff. Measurement protocols should standardise arm use.

Limitations of Indirect Estimation

Sayers and Lewis equations are field-expedient but approximate. Sayers’ peak power equation was derived from a specific population using countermovement jumps; it may overestimate or underestimate power in populations outside its validation range, such as adolescents, masters athletes, or very tall individuals.

The Lewis formula simplifies a complex multi-joint movement into a single work pulse and ignores the horizontal and rotational energy components. Neither equation distinguishes between concentric-only and countermovement jump strategies.

Force plate analysis remains the gold standard, capturing direct ground reaction forces, centre-of-mass velocity, and true power-time curves. For precise monitoring, especially in elite sport, direct dynamometry should supplement or replace regression-based estimates. Nonetheless, the jump height to power conversions offer useful insight when force plates are unavailable.

Interpreting the Full Biomechanical Profile

A 24-inch vertical jump delivers more than just a ranking on a normative chart. It simultaneously implies a takeoff velocity of 3.46 m/s, a hang time of 0.71 seconds, peak power near 5300 W, and a ground reaction impulse exceeding 280 N·s.

Tracking these derived metrics over time reveals whether improvements in jump height come from increased maximal force, enhanced rate of force development, or reduced body mass—all of which steer training decisions in different directions.

Repeated assessments that include body weight, standing reach, and maximum jump reach allow computation of relative power trends and power-to-weight ratios. An athlete who gains 5 lb of lean mass while maintaining the same jump height has actually increased absolute power, a shift that a raw height measurement alone would mask.