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SCIENCE · INVESTIGATE AND EXPLAIN

Evaluate circular-orbit evidence and limits

Audit an analytic solution while distinguishing internal checks from real trajectory validation.

Learning outcome: Write a bounded model conclusion and specify independent observations needed to evaluate a circular approximation.

Starting recap

This model analytically selects a circular orbit; changing radius is not an engine burn or transfer trajectory.

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Try

Recomputing circumference divided by speed checks the period calculation but does not validate it against a tracked satellite.

Open the experiment

Predict

Does a perfect circular path on the diagram show that a real spacecraft follows this approximation?

Experiment

Build a ledger checking period, inward acceleration and angle at the default radius. Then identify evidence missing for a real tracking or transfer claim.

Compare gravity-driven circular orbits

Worked teaching model · synthetic values · Spherical Earth with mean radius 6371 km and rounded GM = 398600 km³/s²; negligible satellite mass. Both circular solutions begin on +x and move counterclockwise in an inertial plane. The dashed reference is at two Earth radii. Changing radius selects a different circular solution, not a maneuver. No drag, thrust, Earth rotation, oblateness, other bodies or measured satellite tracking is included.

Reset keeps your prediction, captures and practice history.

Earth-centered inertial plane · same elapsed time for both orbitsSolid circle: selected · dashed circle: reference at 2 Earth radii-8-8-4-404488EarthDirection-only insetvav: velocity · a: accelerationPosition axes in Earth radii · Earth to scale; satellite symbols enlargedArrows: tangent velocity 8 px/(km/s) · inward acceleration 3 px/(m/s²)

The gold circle is the selected satellite; the outlined square is the reference. They overlap when radius is 2 Earth radii. Arrow lengths use different, fixed scales because velocity and acceleration have different units; compare their directions, not their lengths to one another. At large radii the acceleration arrow becomes very short. The inset gives both arrows equal lengths to show direction only: solid v for velocity, dashed a for acceleration. Its lengths do not compare magnitudes; the ledger retains all components.

Orbital period increases faster than radiusAnalytic circular solutions, not observations or a fitted dataset050010001500200012345678Center-to-center radius / Earth radius · period in minutes
Selected circular solution and fixed two-radius reference
QuantitySelectedReference
Radius from Earth center12742.0 km12742.0 km
Altitude above spherical surface6371.0 km6371.0 km
Inward gravitational acceleration2.4551 m/s²2.4551 m/s²
Circular speed5.5931 km/s5.5931 km/s
Orbital period238.570 min238.570 min
Total angle since starting position45.27°45.27°
Current orientation, modulo 360°45.27°45.27°
Velocity components (x, y)(-3.9735, 3.9362) km/s(-3.9735, 3.9362) km/s
Acceleration components (x, y)(-1.7278, -1.7441) m/s²(-1.7278, -1.7441) m/s²

Selected/reference ratios: radius 1.000, gravity 1.000, speed 1.000, period 1.000. Try radii 2 and 4: doubling center-to-center radius quarters gravity, multiplies speed by 1/√2 and period by √8. Doubling altitude is a different change.

Using μ = GM = 398600 km³/s² and radius r in km: gravity = μ/r² in km/s² (multiply by 1000 for m/s²); circular speed v = √(μ/r); period T = 2πr/v in seconds. Inward acceleration v²/r equals gravitational acceleration. The satellite falls continuously around Earth; free fall is not absence of gravity.

Time selects an analytic snapshot with no integration error or autoplay. Both satellites begin at +x with counterclockwise velocity. Radius changes create separate circular initial conditions; they do not simulate firing a rocket, an elliptical transfer, a launch or an operational satellite trajectory. This inertial view has no rotating surface or ground track.

Radius 12742.0 km from center; altitude 6371.0 km. Circular speed 5.593 km/s; period 238.57 min.

Gravity supplies inward acceleration 2.455 m/s². After 30 min: 45.27° total angle and 45.27° orientation. Relative to the two-radius reference: period ×1.000, speed ×1.000. Constant speed does not mean constant velocity or zero acceleration.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Separate a solved model from a measured trajectory

A smooth orbit can look convincing without providing independent evidence. This lab evaluates the circular solution analytically: radius stays fixed, speed is selected for that radius, and angle advances according to the computed period. The path is circular because that solution is built into the calculation, not because observations were supplied and showed a circular orbit.

The physical relationships express gravity and circular motion. Their implementation can still contain mistakes, so numerical consistency checks are useful. They answer whether the program follows its equations. Testing how accurately those equations describe a particular spacecraft requires measurements and a defined prediction task.

NASA’s gravity and mechanics chapter discusses orbital free fall and real effects such as atmospheric drag. This lab deliberately uses a spherical Earth, negligible spacecraft mass and an isolated, drag-free circular orbit. It includes no thrust, third-body perturbation, Earth flattening or elliptical solver.

Audit a worked output

At radius 2R, record radius 12742 km, altitude 6371 km, speed about 5.5931 km/s, period about 238.5703 minutes and acceleration about 2.4551 m/s². Use the reported speed to calculate circumference divided by speed. Remember that distance in kilometers divided by km/s gives seconds, which must be divided by 60 for minutes.

Next compute v²/r using the same kilometer units, then multiply by 1000 to express acceleration in m/s². It should agree with the gravitational acceleration, within rounding. Finally, calculate 360 × 30/238.5703 to predict the angle at 30 minutes. These three checks link distance, speed, acceleration and time instead of testing only one displayed number.

Keep a ledger headed expected relationship, independent arithmetic and displayed result. Here “independent arithmetic” means your separate calculation, not independent physical observations. Rounding a displayed speed can produce a small mismatch even when the underlying calculation is consistent; record your precision before declaring a failure.

Look for conclusions the display cannot support

The reference radius is fixed at 2R, and both modeled objects begin on the positive horizontal axis. The comparison is constructed, not a pair of actual satellites launched together. A radius adjustment selects another circular solution and immediately supplies its corresponding speed. It does not compute the energy, engine timing or intermediate path of a transfer.

The plane is inertial for this idealized calculation, with no rotation of Earth or mapping to geographic coordinates. The diagram therefore cannot predict which city lies below the object, when an observer will see it, or when it crosses a particular longitude. A completed revolution is not a ground-track forecast.

The spherical radius and rounded μ are based on the NASA Earth fact sheet. That page also distinguishes equatorial and polar radius. Choosing a mean-radius sphere makes the exercise tractable; it does not establish that Earth’s real shape has no dynamical consequences.

Design evidence for a bounded real question

Suppose the question is whether an observed object’s motion over a short interval is adequately described by a circular approximation. You would need timestamped position estimates in a stated reference frame, their uncertainties, and a way to estimate orbital parameters without using every observation for both fitting and evaluation.

Write a plan that fits on one page. Reserve later observations before adjusting parameters, predict positions at their timestamps, and compare position residuals against the stated uncertainties. Persistent structured residuals could motivate a less restrictive model, but one residual pattern would not by itself identify drag or a particular external force. Check time standards, units and frame definitions before assigning a physical cause.

No such observations are loaded here. Your plan is proposed evidence collection, not a completed validation exercise. Keep that distinction in the conclusion accompanying your model ledger.

Transfer by repairing a mission claim

A report says: “Changing the radius from 2R to 4R showed that a spacecraft can reach the higher orbit by instantly reducing its speed to 3.95 km/s.” Rewrite the claim and identify the missing calculation.

Check the orbit-evidence transfer

The model compares separate ideal circular orbits: the 4R circle requires about 3.95 km/s. It does not show a transfer from 2R. Evaluating that maneuver requires a trajectory and thrust or impulse calculation, with appropriate initial conditions and forces, rather than an instantaneous radius selection.

Apply

Changing the radius slider from 2R to 4R demonstrates:

Public practice checks a specific claim. It does not establish independent mastery.

Separate equation checks, proposed held-out observations, omitted forces and unmodeled maneuvers in your conclusion.

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

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