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Cambridge A Levels A2 Physics Chapter 13 Gravitational Fields R53,82   Add to cart

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Cambridge A Levels A2 Physics Chapter 13 Gravitational Fields

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Chapter 22 Gravitational Fields: 24 pages Sick of reading textbooks full of nonsense and gibberish? Hard to study with your teacher's notes? Lazy to do your own notes? Can't find any online notes that are extensive enough and always leave out something from the syllabus? Look no further !! Th...

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  • May 19, 2024
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Chapter 13 Gravitational Fields

Field: a region of space in which an object experiences a force
Gravitational Field
A region of space in which a mass experiences a force.


Newton’s Law of Gravitation

The gravitational force between two-point masses is directly proportional to the product
of their masses and inversely proportional to the square of their separation.



2-point masses: • •

The law still holds when the size
of the masses (diameter) is
small compared to their
separation (r).




𝐹 ∝ 𝑚1 𝑚2
𝑚1 𝑚2
1 𝐹∝
𝐹∝ 2 𝑟2
𝑟



𝑮𝒎𝟏 𝒎𝟐
𝑭=
𝒓𝟐


Universal Gravitational Constant, G = 6.6710-11 Nm2kg-2

,Gravitational Field Strength
Gravitational Field Strength (at a point in a gravitational field)

Force per unit mass at a given point gravitational field.


(vector quantity)
𝑭
𝒈= Unit: N kg-1
𝒎

𝑔 = gravitational field strength (Nkg-1)
𝐹 = gravitational force (N)
𝑚 = mass of test mass in a gravitational field generated by a source mass (kg)




Representing Gravitational Fields




Radial Gravitational Field Uniform Gravitation Field
(Non-uniform field)


Arrows of the field lines: the direction of the gravitational force on a mass placed in the field.
Spacing of the field lines: indicates the gravitational field strength, spacing, strength.

, Gravitational Field Strength in a Radial Gravitational Field




𝐺𝑀𝑚
Force acting on test mass, 𝐹 = 𝑟2
𝐹
Force per unit mass (gravitational field strength) at location of test mass, 𝑔 = 𝑚

𝐺𝑀𝑚
2
𝑔= 𝑟
𝑚
𝐺𝑀
𝑔=
𝑟2
Gravitational Field Strength (In a radial gravitational field),

𝑮𝑴 Source mass
𝒈=
𝒓𝟐

𝐹
𝑔=
𝑚 Test mass

Graph of Radial Gravitational Field Strength




𝑔∝𝑟 1
𝑔∝
𝑟2 r0 → g0
1
2ro → 4g0

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