Gravitation Class Notes PDF Arjuna JEE 2025

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.

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## 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.