Claim status
Absent gravity not supported
In the record
Orbital free-fall explanation documented by NASA
Testable
Gravitational acceleration as a function of distance from Earth’s centre
Method
Inverse-square gravity for a spherical Earth
SPACE & FLIGHT / CASE FILE

Gravity at ISS altitude: 8.69 m/s², 88.53% of surface

At station altitude Earth's gravity is still 8.69 m/s², or 88.53% of its surface value, pulling 695.5 N on the example mass.

Astronauts float through a cabin while Earth is visibly nearby. That apparent contradiction is real: the planet’s gravitational field is still strong at ordinary orbital altitudes. The missing quantity is the force from the floor. An astronaut, a loose object and the spacecraft can all fall together while gravity continues to accelerate them.

Run the calculation
Earth above a cobalt lunar horizonThe view from here is not the whole picture.
01 / THE CLAIM

Floating is mistaken for a gravity-free location

The claim is that orbital footage must be staged because astronauts float close to a planet that should still pull them downward. Sometimes it appears in the opposite form: the footage is explained by saying that there is simply no gravity in space. Both versions assign the visible floating to a missing gravitational field.

The observation worth keeping is that ordinary orbital altitude does not carry a spacecraft very far from Earth’s centre compared with Earth’s own radius. Gravity should remain substantial there. A successful explanation has to retain that pull while explaining why the astronaut does not stand heavily on the cabin floor.

02 / THE CASE

A scale needs something to push against

When a person stands on the ground, the ground prevents free fall and exerts an upward contact force. A bathroom scale responds to that support force. Remove the support and the person can accelerate under gravity while the scale reading approaches zero. A zero reading is therefore not a direct measurement of a zero gravitational field.

NASA creates brief periods of reduced apparent weight in falling experiments and aircraft following appropriate trajectories. Those facilities operate close to Earth. They demonstrate that free fall can produce floating without transporting an experiment to a remote place where the planet’s attraction has nearly vanished.

An orbit applies the same principle over a sustained path. The spacecraft has sideways motion as gravity changes its direction toward Earth. Its occupants share the motion. A released object initially shares the cabin’s trajectory and does not immediately drop toward a floor that is itself falling. Small relative motions can remain, which is why the useful term is microgravity.

03 / THE COMPUTATION

Measure the distance from the centre

The calculation treats Earth as a nonrotating sphere with JPL’s mean radius and gravitational parameter. Add the selected altitude to the radius, square that total distance, and divide the gravitational parameter by the result. This gives gravitational acceleration. Using the same model at the surface provides a consistent comparison without mixing a local surface measurement into a spherical calculation.

At the opening assumption of 400 kilometres altitude, the result is about 8.69 metres per second squared, or 88.53 percent of the model’s surface value. Changing the example mass does not change either number. It changes the gravitational force, found by multiplying the mass by that acceleration.

For the assumed 80-kilogram mass, the gravitational force is about 696 newtons. That is also the support force required to hold the mass stationary at this height in the nonrotating model. It is not the expected reading of a scale freely falling alongside the mass. Calling the calculated force an onboard scale reading would reintroduce the original mistake.

The altitude control makes the inverse-square relationship visible. Doubling altitude does not quarter gravity, because altitude is only the extra distance above the surface. To quarter the spherical field, the entire distance from Earth’s centre must double. The centre-to-object distance is the quantity that belongs in the denominator.

RUN THE NUMBERS

How much gravity remains at this altitude?

Choose height above a spherical, nonrotating Earth and an example mass. The force output is gravitational pull, not a scale reading in a freely falling cabin.

Calculation inputs
km

Your altitude assumption. Higher altitude weakens gravity through the square of distance from Earth’s centre.

kg

Your mass assumption. Doubling mass doubles force but leaves gravitational acceleration unchanged.

Share of spherical surface gravity88.53%

Compared with the same nonrotating spherical model at zero altitude.

Gravitational acceleration8.69 m/s²

The field still accelerates the spacecraft and its freely falling contents.

Gravitational pull on the example mass695.5 N

A freely falling scale does not support this force; this is not its reading.

Working tape
  1. Earth radius + altitude6,371.0084 + 400 = 6,771.0084
  2. Square the distance from Earth’s centre6,771.0084 ^ 2 = 45,846,554.752871
  3. Gravitational parameter ÷ distance squared398,600.435507 ÷ 45,846,554.752871 = 0.008694
  4. Convert acceleration to metres per second squared0.008694 × 1,000 = 8.694229
  5. Earth radius ÷ orbital radius6,371.0084 ÷ 6,771.0084 = 0.940925
  6. Square the radius ratio0.940925 ^ 2 = 0.885339
  7. Fraction × 1000.885339 × 100 = 88.533911
  8. Example mass × gravitational acceleration80 × 8.694229 = 695.538302
04 / THE FINDING

Strong gravity and floating belong together

At the assumed 400-kilometre altitude, 88.53 percent of the spherical model’s surface gravity remains. An 80-kilogram mass experiences about 696 newtons of gravitational pull. The spacecraft and its contents share the resulting acceleration, so a loose object can appear to hang beside its observer.

The missing force is support from the floor. A scale held stationary at that height would have to support the mass against gravity; a scale falling alongside it does not. Strong gravity and reduced apparent weight therefore belong in the same explanation. Orbital floating follows from their shared fall, even while Earth continues to pull strongly on everything in the cabin.

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