Commander David Scott conducting an experiment during the Apollo 15 moon landing.

Free fall is any motion of a body where its weight is the only force acting upon it. These conditions produce an inertial trajectory so long as gravity remains the only force. Since this definition does not specify velocity, it also applies to objects initially moving upward. Since free fall in the absence of forces other than gravity produces weightlessness or "zero-g," sometimes any condition of weightlessness due to inertial motion is referred to as free-fall. This may also apply to weightlessness produced because the body is far from a gravitating body.

Although strict technical application of the definition excludes motion of an object subjected to other forces such as aerodynamic drag, in nontechnical usage, falling through an atmosphere without a deployed parachute, or lifting device, is also often referred to as free fall. The drag forces in such situations prevent them from producing full weightlessness, and thus a skydiver's "free fall" after reaching terminal velocity produces the sensation of the body's weight being supported on a cushion of air.

Examples [link]

A video showing objects free-falling 215 feet (65 m) down a metal well, a type of drop tube

Examples of objects in free fall include:

• A spacecraft (in space) with propulsion off (e.g. in a continuous orbit, or on a suborbital trajectory (ballistics) going up for some minutes, and then down).
• An object dropped at the top of a drop tube.
• An object thrown upwards or a person jumping off the ground at low speed (i.e. as long as air resistance is negligible in comparison to weight).

Technically, an object is in free fall even when moving upwards or instantaneously at rest at the top of its motion. If gravity is the only influence acting, then the acceleration is always downward and has the same magnitude for all bodies, commonly denoted Failed to parse (Missing texvc executable; please see math/README to configure.): g .

Since all objects fall at the same rate in the absence of other forces, objects and people will experience weightlessness in these situations.

Examples of objects not in free fall:

• Flying in an aircraft: there is also an additional force of lift.
• Standing on the ground: the gravitational force is counteracted by the normal force from the ground.
• Descending to the Earth using a parachute, which balances the force of gravity with an aerodynamic drag force (and with some parachutes, an additional lift force).

The example of a falling skydiver who has not yet deployed a parachute is not considered free fall from a physics perspective, since they experience a drag force which equals their weight once they have achieved terminal velocity (see below). However, the term "free fall skydiving" is commonly used to describe this case in everyday speech, and in the skydiving community. It is not clear, though, whether the more recent sport of wingsuit flying fits under the definition of free fall skydiving.

Measured fall time of a small steel sphere falling from various heights. The data is in good agreement with the predicted fall time of Failed to parse (Missing texvc executable; please see math/README to configure.): \sqrt{2h/g} , where h is the height and g is the free-fall acceleration due to gravity.

Near the surface of the Earth, an object in free fall in a vacuum will accelerate at approximately 9.8 m/s², independent of its mass. With air resistance acting upon an object that has been dropped, the object will eventually reach a terminal velocity, around 56 m/s (200 km/h or 120 mph) for a human body. Terminal velocity depends on many factors including mass, drag coefficient, and relative surface area and will only be achieved if the fall is from sufficient altitude.

Free fall was demonstrated on the moon by astronaut David Scott on August 2, 1971. He simultaneously released a hammer and a feather from the same height above the moon's surface. The hammer and the feather both fell at the same rate and hit the ground at the same time. This demonstrated Galileo's discovery that in the absence of air resistance, all objects experience the same acceleration due to gravity. (On the Moon, the gravitational acceleration is much less than on Earth, approximately 1.6 m/s²).

Free fall in Newtonian mechanics [link]

Uniform gravitational field without air resistance [link]

This is the "textbook" case of the vertical motion of an object falling a small distance close to the surface of a planet. It is a good approximation in air as long as the force of gravity on the object is much greater than the force of air resistance, or equivalently the object's velocity is always much less than the terminal velocity (see below).

Failed to parse (Missing texvc executable; please see math/README to configure.): v(t)=-gt+v_{0}\,

Failed to parse (Missing texvc executable; please see math/README to configure.): y(t)=-\frac{1}{2}gt^2+v_{0}t+y_0

where

Failed to parse (Missing texvc executable; please see math/README to configure.): v_{0}\,

is the initial velocity (m/s).

Failed to parse (Missing texvc executable; please see math/README to configure.): v(t)\,

is the vertical velocity with respect to time (m/s).

Failed to parse (Missing texvc executable; please see math/README to configure.): y_0\,

is the initial altitude (m).

Failed to parse (Missing texvc executable; please see math/README to configure.): y(t)\,

is the altitude with respect to time (m).

Failed to parse (Missing texvc executable; please see math/README to configure.): t\,

is time elapsed (s).

Failed to parse (Missing texvc executable; please see math/README to configure.): g\,

is the acceleration due to gravity (9.81 m/s2 near the surface of the earth).

Uniform gravitational field with air resistance [link]

Acceleration of a small meteoroid when entering the Earth's atmosphere at different initial velocities.

This case, which applies to skydivers, parachutists or any body of mass, Failed to parse (Missing texvc executable; please see math/README to configure.): m , and cross-sectional area, Failed to parse (Missing texvc executable; please see math/README to configure.): A , with Reynolds number well above the critical Reynolds number, so that the air resistance is proportional to the square of the fall velocity, Failed to parse (Missing texvc executable; please see math/README to configure.): v , has an equation of motion

Failed to parse (Missing texvc executable; please see math/README to configure.): m\frac{dv}{dt}=\frac{1}{2} \rho C_{\mathrm{D}} A v^2 - mg \, ,

where Failed to parse (Missing texvc executable; please see math/README to configure.): \rho

is the air density and Failed to parse (Missing texvc executable; please see math/README to configure.): C_{\mathrm{D}}
is the drag coefficient, assumed to be constant although in general it will depend on the Reynolds number.

Assuming an object falling from rest and no change in air density with altitude, the solution is:

Failed to parse (Missing texvc executable; please see math/README to configure.): v(t) = -v_{\infty} \tanh\left(\frac{gt}{v_\infty}\right),

where the terminal speed is given by

Failed to parse (Missing texvc executable; please see math/README to configure.): v_{\infty}=\sqrt{\frac{2mg}{\rho C_D A}} \, .

The object's speed versus time can be integrated over time to find the vertical position as a function of time:

Failed to parse (Missing texvc executable; please see math/README to configure.): y = y_0 - \frac{v_{\infty}^2}{g} \ln \cosh\left(\frac{gt}{v_\infty}\right).

When the air density cannot be assumed to be constant, such as for objects or skydivers falling from high altitude, the equation of motion becomes much more difficult to solve analytically and a numerical simulation of the motion is usually necessary. The figure shows the forces acting on meteoroids falling through the Earth's upper atmosphere. HALO jumps, including Col. Joe Kittinger's record jump (see below) and the planned Le Grand Saut also belong in this category.^[1]

Inverse-square law gravitational field [link]

It can be said that two objects in space orbiting each other in the absence of other forces are in free fall around each other, e.g.that the Moon or an artificial satellite "falls around" the Earth, or a planet "falls around" the Sun. Assuming spherical objects means that the equation of motion is governed by Newton's Law of Universal Gravitation, with solutions to the gravitational two-body problem being elliptic orbits obeying Kepler's laws of planetary motion. This connection between falling objects close to the Earth and orbiting objects is best illustrated by the thought experiment Newton's cannonball.

The motion of two objects moving radially towards each other with no angular momentum can be considered a special case of an elliptical orbit of eccentricity e = 1 (radial elliptic trajectory). This allows one to compute the free-fall time for two point objects on a radial path. The solution of this equation of motion yields time as a function of separation:

Failed to parse (Missing texvc executable; please see math/README to configure.): t(y)= \sqrt{ \frac{ {y_0}^3 }{2\mu} } \left(\sqrt{\frac{y}{y_0}\left(1-\frac{y}{y_0}\right)} + \arccos{\sqrt{\frac{y}{y_0}}} \right)

where

t is the time after the start of the fall

y is the distance between the centers of the bodies

y₀ is the initial value of y

μ = G(m₁ + m₂) is the standard gravitational parameter.

Substituting y=0 we get the free-fall time.

The separation as a function of time is given by the inverse of the equation. The inverse is represented exactly by the analytic power series:

Failed to parse (Missing texvc executable; please see math/README to configure.): y( t ) = \sum_{n=1}^{ \infty } \left[ \lim_{ r \to 0 } \left( {\frac{ x^{ n }}{ n! }} \frac{\mathrm{d}^{\,n-1}}{\mathrm{ d } r ^{\,n-1}} \left[ r^n \left( \frac{ 7 }{ 2 } ( \arcsin( \sqrt{ r } ) - \sqrt{ r - r^2 } ) \right)^{ - \frac{2}{3} n } \right] \right) \right]

Evaluating this yields:

Failed to parse (Missing texvc executable; please see math/README to configure.): y(t)=y_0 \left( x - \frac{1}{5} x^2 - \frac{3}{175}x^3 - \frac{23}{7875}x^4 - \frac{1894}{3931875}x^5 - \frac{3293}{21896875}x^6 - \frac{2418092}{62077640625}x^7 - \cdots \right) \

where

Failed to parse (Missing texvc executable; please see math/README to configure.): x = \left[\frac{3}{2} \left( \frac{\pi}{2}- t \sqrt{ \frac{2\mu}{ {y_0}^3 } } \right) \right]^{2/3}

For details of these solutions see "From Moon-fall to solutions under inverse square laws" by Foong, S. K., in European Journal of Physics, v29, 987-1003 (2008) and "Radial motion of Two mutually attracting particles", by Mungan, C. E., in The Physics Teacher, v47, 502-507 (2009).

Free fall in General Relativity [link]

The experimental observation that all objects in free fall accelerate at the same rate, as noted by Galileo and confirmed to high accuracy by modern forms of the Eötvös experiment, is the basis of the Equivalence Principle, on which Einstein's theory of general relativity relies. An alternative statement of this law, as can be seen from Newton's 2nd law applied to free fall above, is that the gravitational and the inertial mass of any object are the same.

Record free fall parachute jumps [link]

Joseph Kittinger starting his record-breaking skydive.

According to the Guinness Book of Records, Eugene Andreev (USSR) holds the official FAI record for the longest free-fall parachute jump after falling for 80,380 ft (24,500 m) from an altitude of 83,523 ft (25,460 m) near the city of Saratov, Russia on November 1, 1962. Though later jumpers would ascend higher, Andreev's record was set without the use of a drogue chute during the jump.^[2]

During the late 1950s, Captain Joseph Kittinger of the United States was assigned to the Aerospace Medical Research Laboratories at Wright-Patterson AFB in Dayton, Ohio. For Project Excelsior (meaning "ever upward", a name given to the project by Colonel John Stapp), as part of research into high altitude bailout, he made a series of three parachute jumps wearing a pressurized suit, from a helium balloon with an open gondola.

The first, from 76,400 feet (23,290 m) in November, 1959 was a near tragedy when an equipment malfunction caused him to lose consciousness, but the automatic parachute saved him (he went into a flat spin at a rotational velocity of 120 rpm; the g-force at his extremities was calculated to be over 22 times that of gravity, setting another record). Three weeks later he jumped again from 74,700 feet (22,770 m). For that return jump Kittinger was awarded the A. Leo Stevens parachute medal.

On August 16, 1960 he made the final jump from the Excelsior III at 102,800 feet (31,330 m). Towing a small drogue chute for stabilization, he fell for 4 minutes and 36 seconds reaching a maximum speed of 614 mph (988 km/h) [1] before opening his parachute at 14,000 feet (4,270 m). Pressurization for his right glove malfunctioned during the ascent, and his right hand swelled to twice its normal size.^[3] He set records for highest balloon ascent, highest parachute jump, longest drogue-fall (4 min), and fastest speed by a human through the atmosphere.^[4]

The jumps were made in a "rocking-chair" position, descending on his back, rather than the usual arch familiar to skydivers, because he was wearing a 60-lb "kit" on his behind and his pressure suit naturally formed that shape when inflated, a shape appropriate for sitting in an airplane cockpit.

For the series of jumps, Kittinger was decorated with an oak leaf cluster to his Distinguished Flying Cross and awarded the Harmon Trophy by President Dwight Eisenhower.

Surviving falls [link]

The severity of injury increases with the height of a free fall, but also depends on body and surface features and the manner of body impacts on to the surface.^[5] The chance of surviving increases if landing on a surface of high deformity, such as snow or water.^[5]

Overall, the height at which 50% of children die from a fall is between four and five storey heights above the ground.^[6]

JAT stewardess Vesna Vulović survived a fall of 33,000 feet (10,000 m)^[7] on January 26, 1972 when she was aboard JAT Flight 367. The plane was brought down by explosives over Srbská Kamenice in the former Czechoslovakia (now Czech Republic). The Serbian stewardess suffered a broken skull, three broken vertebrae (one crushed completely), and was in a coma for 27 days. In an interview she commented that, according to the man who found her, "...I was in the middle part of the plane. I was found with my head down and my colleague on top of me. One part of my body with my leg was in the plane and my head was out of the plane. A catering trolley was pinned against my spine and kept me in the plane. The man who found me, says I was very lucky. He was in the German Army as a medic during World War Two. He knew how to treat me at the site of the accident." ^[8]

In World War II there were several reports of military aircrew surviving long falls: Nick Alkemade, Alan Magee, and Ivan Chisov all fell at least 5,500 metres (18,000 ft) and survived.

Freefall is not to be confused with individuals who survive instances of various degrees of controlled flight into terrain. Such impact forces affecting these instances of survival differ from the forces which are characterized by free fall.

It was reported that two of the victims of the Lockerbie bombing survived for a brief period after hitting the ground (with the forward nose section fuselage in freefall mode), but died from their injuries before help arrived.^[9]

Juliane Koepcke survived a long free fall resulting from the December 24, 1971, crash of LANSA Flight 508 (a LANSA Lockheed Electra OB-R-941 commercial airliner) in the Peruvian rainforest. The airplane was struck by lightning during a severe thunderstorm and exploded in mid air, disintegrating two miles up. Köpcke, who was 17 years old at the time, fell to earth still strapped into her seat. The German Peruvian teenager survived the fall with only a broken collarbone, a gash to her right arm, and her right eye swollen shut.^[10]

As an example of 'freefall survival' that was not as extreme as sometimes reported in the press, a skydiver from Staffordshire was said to have plunged 6,000 metres without a parachute in Russia and survived. James Boole said he was supposed to have been given a signal by another skydiver to open his parachute, but it came two seconds too late. Mr Boole, who was filming the other skydiver for a television documentary, landed on snow-covered rocks and suffered a broken back and rib.^[11] While he was lucky to survive, this was not a case of true freefall survival, because he was flying a wingsuit, greatly decreasing his vertical speed. This was over descending terrain with deep snow cover, and he impacted while his parachute was beginning to deploy. Over the years other skydivers have survived accidents where the press has reported that no parachute was open, yet they were actually being slowed by a small area of tangled parachute. They might still be very lucky to survive, but an impact at 80 mph is much less severe than the 120 mph that might occur in normal freefall.

See also [link]

• Free-falling aircraft
• Weightlessness
• Terminal velocity
• HALO jump
• g-force
• Microgravity

References [link]

External links [link]

• Unplanned Freefall? A slightly tongue-in-cheek look at surviving free-fall without a parachute.
• Free fall accidents, mathematics of free fall - detailed research on the topic
• Chuteless jump survivors
• "Joseph W. Kittinger and the Highest Step in the World". Greg Kennedy. March 17, 2010. https://stratocat.com.ar/artics/excelsior-e.htm.  detailed account of origins and development of EXCELSIOR project
• The Way Things Fall an educational website

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