OCR A-Level Physics B H557
Planning
Implementing
Analysis
Evaluation
Practical Skills
Use of Apparatus and Techniques
Fundamental Data Analysis
Imaging and Signalling
Sensing
Mechanical Properties of Materials
Waves and Quantum Behaviour
Space, Time and Motion
Creating Models
Out Into Space
Our Place in the Universe
Matter: Very Simple
Matter: Hot or Cold
Electromagnetism
Charge and Field
Probing Deep Into Matter
Ionising Radiation and Risk
Out Into Space
- 9 subtopics
- 27 things to know
- Components 01, 02 and 03
What Out Into Space covers
Out Into Space is examined in all three written papers — the specification states that Components 01, 02 and 03 each assess content from across all the teaching modules, so nothing is confined to one paper. It covers gravitational and kinetic energy changes, motion in a uniform gravitational field, gravitational force and the radial field, gravitational field strength, gravitational potential energy in a radial field, gravitational potential and equipotentials, graphs and diagrams of gravitational fields, angular velocity and motion in a horizontal circle and circular gravitational orbits.
Where it is assessed
Components 01, 02 and 03
Every module can be assessed on any of the three papers.
Check the OCR specification ↗The 9 subtopics
Each one has its own page.
- Gravitational and kinetic energy changesRecall questions on the near-surface potential energy equation, work done by a force, why mass cancels in a landing speed, path independence, and areas under force–distance graphs.Open →
- Motion in a uniform gravitational fieldRecall questions on field lines and equipotentials, showing newtons per kilogram equals metres per second squared, treating projectile motion as two independent directions, and where this approximation fails.Open →
- Gravitational force and the radial fieldRecall questions on F = −GMm/r² and its minus sign, the gravitational constant G, the inverse square law, treating planets as point masses, satellite and sphere force calculations, doubling separation, why everyday attraction is unnoticeable, Newton's third law pairs, radial field lines, a larger planet's surface force, and gravity against the strong nuclear force.Open →
- Gravitational field strengthRecall questions on the defining equation and unit, inverse-square variation around a planet, adding fields from two bodies and where they cancel, apparent weightlessness in orbit, and field-line spacing.Open →
- Gravitational potential energy in a radial fieldRecall questions on E = −GMm/r and why it is negative, the zero at infinite separation, how potential energy changes with distance, satellite and spacecraft calculations, constant energy in a circular orbit, when mgh is enough, escape velocity v = √(2GM/r) and why it does not depend on mass, negative total energy in a bound orbit, and the energy–distance graph.Open →
- Gravitational potential and equipotentialsRecall questions on gravitational potential V = −GM/r and its unit, its link to potential energy, potential as a scalar, the potential at the Earth's surface, equipotential surfaces around a planet and why moving along one needs no work, their relation to field lines, escape energy per kilogram, the energy to move a probe, equipotential spacing, and which way a released mass moves.Open →
- Graphs and diagrams of gravitational fieldsRecall questions on the areas under field– and force–distance graphs, finding force or field from a gradient, estimating an area under a curve, equipotential diagrams, and why potential stays below zero.Open →
- Angular velocity and motion in a horizontal circleRecall questions on angular velocity and its unit, radians in a revolution, ω = 2π/T and v = ωr, centripetal acceleration a = v²/r and its direction, F = mv²/r and F = mrω², why uniform circular motion is accelerated, calculations for a stone, a car and a whirled mass, why centripetal force does no work, and what holds a satellite in orbit.Open →
- Circular gravitational orbitsRecall questions on gravity supplying the centripetal force, deriving orbital speed and the period–radius relation, why satellite mass drops out, geostationary and polar orbits, and decaying low orbits.Open →
What you need to know
Answer each one before you reveal it.
Why is gravitational potential energy defined as negative?
Why can mgh be used near the surface while −GMm/r is needed for a rocket leaving the Earth?
What equation gives the change in gravitational potential energy near the Earth's surface?
What equation gives the gravitational force between two point masses?
What is the field strength at a distance r from a point mass M?
How is gravitational potential related to gravitational potential energy?
How is the gravitational force found from a graph of gravitational potential energy against distance?
How is angular velocity related to the period of the motion?
Why does orbital speed not depend on the mass of the satellite?
A 70 kg climber ascends 12 m. What is the gain in gravitational potential energy?
Why do all objects in free fall near the Earth have the same acceleration?
Why does the radial component of the gravitational force carry a minus sign?
Calculate the gravitational field strength at the surface of an Earth of mass 5.97 × 10²⁴ kg and radius 6.37 × 10⁶ m.
What is the gravitational potential at a distance r from a point mass M?
How is field strength found from a graph of gravitational potential against distance?
How is linear speed related to angular velocity in circular motion?
State the relationship between the period and the radius of a circular orbit in words.
What relationship links work done, force and displacement?
A ball thrown horizontally at 15 m s⁻¹ falls for 2.0 s. How far horizontally does it travel?
State the value and unit of the universal gravitational constant.
What is the field strength 6.37 × 10⁶ m above the surface of the Earth?
What is the gravitational potential energy of a mass m at a distance r from a mass M?
Calculate the gravitational potential at the surface of an Earth with GM = 3.98 × 10¹⁴ N m² kg⁻¹ and radius 6.37 × 10⁶ m.
Why must a change of potential be found as an area rather than by a single multiplication?
What is the expression for centripetal acceleration in terms of speed and radius?
A satellite of orbital radius 6.77 × 10⁶ m travels at 7.7 × 10³ m s⁻¹. What is its period?
Take Out Into Space further
The same content, four other ways.
Commonly confused
Pairs that lose marks when they are blurred together.
Gravitational field strength g vs Gravitational potential V
Gravitational field strength g: the gravitational pull per kilogram on a small test mass at that point, in N kg⁻¹, and a vector directed towards the mass producing it. Gravitational potential V: The work done per kilogram in bringing a small test mass from infinity to that point, in J kg⁻¹, and a scalar that is negative everywhere.
mgh vs −GMm/r
mgh: the change in energy when a mass is raised through a small height near the surface, where the pull per kilogram is effectively constant. −GMm/r: The absolute energy in joules that one particular mass has in a radial field, negative everywhere and rising towards zero at infinity.
Inverse square for force vs Inverse for potential
Inverse square for force: the pull between two masses falls as 1/r², so tripling the separation cuts it to a ninth. Inverse for potential: The energy per kilogram at a point falls as −1/r, so doubling the distance halves it rather than quartering it.
Questions from this topic
Each one with the model answer underneath.
- 1
What equation gives the change in gravitational potential energy near the Earth's surface?
Model answer
The change is ΔE = mgΔh, where g is the gravitational field strength.
- 2
Why is mgh valid only close to the Earth's surface?
Model answer
It assumes the field strength g is constant, which is true only over heights small compared with the radius of the Earth.
- 3
A 70 kg climber ascends 12 m. What is the gain in gravitational potential energy?
Model answer
ΔE = mgh = 70 × 9.81 × 12 = 8.2 × 10³ J.
- 4
What relationship links work done, force and displacement?
Model answer
The work done is ΔE = FΔs, where the displacement is measured along the direction of the force.
- 5
Why is no work done when a force acts at right angles to the motion?
Model answer
There is no displacement in the direction of the force, so the product FΔs along that direction is zero.
- 6
A ball of mass 0.20 kg is dropped from 1.8 m. What is its speed on landing, ignoring air resistance?
Model answer
From mgh = ½mv², v = √(2 × 9.81 × 1.8) = 5.9 m s⁻¹.
What is inside Levo
Six ways to work the same material.
Out Into Space revision questions
- What does Out Into Space cover in OCR A-Level Physics B?
- 9 subtopics: gravitational and kinetic energy changes, motion in a uniform gravitational field, gravitational force and the radial field, gravitational field strength, gravitational potential energy in a radial field, gravitational potential and equipotentials, graphs and diagrams of gravitational fields, angular velocity and motion in a horizontal circle and circular gravitational orbits. Each one has its own page with questions and model answers.
- How is Out Into Space organised?
- By the OCR H557 specification, subtopic by subtopic, so it matches the order you are taught it in.
Every question in Out Into Space, on a schedule.
Attempt a question from memory, write the correct version, then attempt it again. Levo records the jump between your first attempt and your last, and brings each question back on the day you are due to forget it.
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