Gravitation Class Notes PDF Arjuna JEE 2025
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2025
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Rajwant Singh (RJ)
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Summary
These class notes cover gravitation, providing detailed explanations of Newton's law of gravitation and various examples. The notes are targeted towards JEE 2025 aspirants.
Full Transcript
## ARJUNA JEE 2025 - Gravitation **By - Rajwant Singh (RJ)** **Physics Wallah** ### Lecture - 1 ### Topics 1. Newton laws of gravitation 2. Question 3. Gravitational field intensity 3. Questions ### To be Covered: - Vectors - FBD (force) - Circular Motion ### Newton Law's of Gravitation -...
## ARJUNA JEE 2025 - Gravitation **By - Rajwant Singh (RJ)** **Physics Wallah** ### Lecture - 1 ### Topics 1. Newton laws of gravitation 2. Question 3. Gravitational field intensity 3. Questions ### To be Covered: - Vectors - FBD (force) - Circular Motion ### Newton Law's of Gravitation - Two point masses _m_1 & _m_2 are separated by distance _r_. They always attract each other by a force _F_, which is proportional to the product of masses (_m_1_m_2_) and inversely proportional to the square of the distance between them. - **F = Gm<sub>1</sub>m<sub>2</sub>/r<sup>2</sup>** - _G_ = universal gravitational constant = 6.67 x 10<sup>-11</sup> _Nm_<sup>2</sup>/_kg_<sup>2</sup> ### Important Points: 1. Only applicable for point masses. Distributed mass system is not valid. 2. _G_ = universal gravitational constant = 6.67 x 10<sup>-11</sup> _Nm_<sup>2</sup>/_kg_<sup>2</sup> 3. Always attractive force 4. Force is central, meaning it acts along the line joining the center. 5. Action/Reaction pairs ### Gravitational Force is Independent of - The medium between two particles. - Presence of a third particle. ### Fgravitation is a Vector The resultant of force is calculated by using vector laws. ### Examples **a)** - A particle _m_0 is placed at x = 0. - Particles with mass _m_ are placed at x = 1m, 2m, 4m, and 8m etc. - **Find F<sub>net</sub> on _m_0 = ?** - **F<sub>net</sub> = Gm<sub>0</sub>m/1<sup>2</sup> + Gm<sub>0</sub>m/2<sup>2</sup> + Gm<sub>0</sub>m/4<sup>2</sup> + Gm<sub>0</sub>m/6<sup>2</sup> ... = (4/3)Gm<sub>0</sub>m** **b)** - Three masses, _m_, _m_, and _m_0 are placed at the corners of an equilateral triangle of side _l_. - Find _F<sub>net</sub>_ on _m_0. - **F<sub>net</sub> = √3Gm<sub>0</sub>m/l<sup>2</sup>** **c)** - Four equal masses, _m_, are placed at the corners of a square. - Find _F<sub>net</sub>_ on _m_0. - **F<sub>net</sub> = (√2 + 1)Gm<sub>0</sub>m/l<sup>2</sup>** **d)** - Four equal masses, _m_, are placed at the corners of rectangle. - Find _F<sub>net</sub>_ on _m_0. - **F<sub>net</sub> = (2√2 + 5)Gm<sub>0</sub>m/l<sup>2</sup>** **e)** - Four equal masses, _m_, are placed at the corners of a circle, with radius _R_. - Find _F<sub>net</sub>_ on _m_0. - **F<sub>net</sub> = (√2 + 1)Gm<sub>0</sub>m/2R<sup>2</sup>** **f)** - Six equal masses, _m_, are placed on a circle. - Find _F<sub>net</sub>_ on _m_0. - **F<sub>net</sub> = (2 + √3)Gm<sub>0</sub>m/R<sup>2</sup>** **g)** - Multiple masses, _m_, are placed on the circumference of a circle at equal angles. - _m_0 is at the center of the circle. - **F<sub>net</sub> on _m_0 = 0** **h)** - Three equal masses, _m_, are placed at the corners of a triangle. - Find the force on _m_0. - **F = 3Gm<sub>0</sub>m/(2√3)<sup>2</sup>** **i)** - Four equal masses, _m_, are placed at the corners of a square. - Find the force on _m_0. - **F<sub>net</sub> on _m_0 = 0** **j)** - Five equal masses, _m_, are placed at the corners of a regular pentagon. - Find the force on _m_0. - **F<sub>net</sub> on _m_0 = 0** **k)** - A regular pentagon with five masses, _m_. - Find the force on _m_0. - **F<sub>net</sub> on _m_0 = Gm<sub>0</sub>m/a<sup>2</sup>** - **Concept of Broken Symmetry** - When a particle is removed from the pentagon , the symmetry breaks and there is a net attraction between the particles. **l)** - Twelve equal masses, _m_. - Find the force on _m_0. - **F<sub>net</sub> on _m_0 = Gm<sub>0</sub>m/R<sup>2</sup>** **m)** - A mass, _M_, is broken into two parts. - The two parts are separated by a distance _r_. - **Find the force between the two part.** - **The force is maximum when the mass is broken into two equal parts (m = M/2).** ### Null Point Problems **Calculation of Null Point** - Point where force = 0 **Null Vector** - Magnitude: 0 - Direction: not defined - **Null point is obtained between the line joining the masses.** **a)** - Masses _m_ and _m_ are separated by a distance _d_. - A mass, _m_0, is placed at a distance _x_ from _m_ and a distance _d-x_ from _m_. - **Find the value of _x_ so that the net force on _m_0 is 0** - **x = d/2** **Generalised Formula for Null Point** - **x = d√n/(√n + 1)** - **Always towards the smaller mass** **b)** - A mass of 4_m_ is placed at one end of a line segment with a length _d_. - A mass of 5_m_ is placed at the other end of the line segment. - Find the Null point. - **x = d/√5+1 = 2d/√5+2** **c)** - Two equal masses, _m_, are fixed at a distance _d_. - A mass _m_0 is placed at a distance _x_ from the midpoint of the line segment. - Find the net force on _m_0 and find at what value of _x_ the force will be maximum. - **F<sub>net</sub> = 2Gm<sub>0</sub>m.x/(d<sup>2</sup> + x<sup>2</sup>)<sup>3/2</sup>** - **The force is maximum at x = d/√2** **HW** - A mass, _m_0, is placed at the centroid of an equilateral triangle, while three equal masses, _m_, are placed at the corner of the triangle. Find the net force on _m_0. - A mass _m_0_ is placed at the center of a square. Four equal masses, _m_, are placed at the corners of the square. Find the net force on _m_0. - A mass, _m_0, is placed at the center of a ring with radius _R_. The mass, _m_, is distributed uniformly across the circumference of the ring. Find the net force on _m_0.