3.3 Gravitational and Electric Forces

Gravitational and Electric Forces Gravitational and electric forces are fundamental interactions that act between objects: Gravitational Force: An attractive force between masses, proportional to their masses and inversely proportional to the square of their distance ( 𝐹 = 𝐺 π‘š 1 π‘š 2 π‘Ÿ 2 F=G r 2 m 1 ​ m 2 ​ ​ ). Electric Force: A force between charged particles, which can be attractive or repulsive, depending on the charges, and follows Coulomb’s law ( 𝐹 = π‘˜ π‘ž 1 π‘ž 2 π‘Ÿ 2 F=k r 2 q 1 ​ q 2 ​ ​ ). Both forces decrease with distance and play a key role in the structure and dynamics of the universe.

3.3 Gravitational and Electric Forces: Understanding the Fundamentals


Gravitational Force: The Universal Attraction

Gravity is the force by which one object with mass attracts another object with mass. From keeping the planets in orbit to shaping the vast structures of galaxies, gravitational force governs many phenomena in the universe.

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What is Gravitational Force?

Gravitational force is always attractive and acts at a distance, making it a long-range force. Unlike contact forces, gravity does not require objects to touch for its effects to be felt.


Equation for Gravitational Force

The force of gravity on an object near the Earth’s surface is calculated using:

Fg=mβ‹…gF_g = m \cdot g

Where:


  • Fgis the force of gravity (N),

  • mm

    is the mass of the object (kg),


  • gg

    is the acceleration due to gravity (9.8 m/s2 on Earth).

This equation shows that the greater the mass of an object, the stronger the gravitational force acting on it.

Key Insight: The gravitational force becomes significant only when the masses of objects are very large, such as planets or stars.


Newton’s Universal Law of Gravitation

Newton’s Law explains that every particle in the universe attracts every other particle. The gravitational force is:

Fg=Gm1β‹…m2r2F_g = G \frac{{m_1 \cdot m_2}}{{r^2}}

Where:


  • FgF_g

    is the gravitational force (N),


  • GG

    is the gravitational constant (6.67Γ—

    10βˆ’11 Nm2/kg26.67 \times 10^{-11} \, \text{Nm}^2/\text{kg}^2

  • m1,m2m_1, m_2

    are the masses of the objects (kg),


  • rr

    is the distance between the centers of the masses (m).


Key Relationships in Newton’s Law

  1. Mass and Gravitational Force:

    • The force is directly proportional to the product of the masses
      m1β‹…m2​
    • Larger masses result in stronger gravitational attraction.
  2. Distance and Gravitational Force:

    • The force is inversely proportional to the square of the distance
      1/r21/r^2
    • Doubling the distance decreases the force to one-fourth.

Gravitational Constant GG

Β 

The small value of

GG

explains why gravitational forces are typically weak unless very large masses are involved. For instance, while a pencil exerts a gravitational pull on you, it is negligible compared to Earth’s pull due to the pencil’s small mass.


Applications of Gravitational Force

  • Orbits: Gravity keeps planets orbiting the Sun and moons orbiting planets.
  • Galaxies: Gravity holds stars and planetary systems together within galaxies.
  • Comets: Gravity governs the motion of comets around stars.
  • Large-Scale Universe: Gravitational forces shape the structure and behavior of galaxy clusters.

Practice Problems

Problem 1:

Two objects with masses of 10 kg and 5 kg are 3 meters apart. What is the gravitational force between them?

  • a)
    0.22 N0.22 \, \text{N}
  • b)
    2.2 N2.2 \, \text{N}
  • c)
    22 N22 \, \text{N}
  • d)
    220 N220 \, \text{N}

Answer: a)

0.22 N0.22 \, \text{N}

Explanation:

F=Gm1β‹…m2r2=(6.67Γ—10βˆ’11)(10)(5)32=0.22 N


Problem 2:

A planet with a mass of

5Γ—1024 kg5 \times 10^{24} \, \text{kg}

Β is

1.5Γ—1011 m1.5 \times 10^{11} \, \text{m}

Β away from a star with a mass of

2Γ—1030 kg2 \times 10^{30} \, \text{kg}

. What is the gravitational force between them?

  • a)
    2.22Γ—1011 N2.22 \times 10^{11} \, \text{N}
  • b)
    2.22Γ—1013 N2.22 \times 10^{13} \, \text{N}
  • c)
    2.22Γ—1015 N2.22 \times 10^{15} \, \text{N}
  • d)
    2.22Γ—1017 N2.22 \times 10^{17} \, \text{N}

Answer: d)

2.22Γ—1017 N2.22 \times 10^{17} \, \text{N}

Explanation:

F=Gm1β‹…m2r2=(6.67Γ—10βˆ’11)(5Γ—1024)(2Γ—1030)(1.5Γ—1011)2=2.22Γ—1017 N


Problem 3:

A satellite with a mass of

500 kg500 \, \text{kg}

is located

1000 km1000 \, \text{km}

from the center of Earth (

5.97Γ—1024 kg5.97 \times 10^{24} \, \text{kg}

). What is the gravitational force acting on the satellite?

  • a)
    1.96Γ—104 N1.96 \times 10^{4} \, \text{N}
  • b)
    3.92Γ—104 N3.92 \times 10^{4} \, \text{N}
  • c)
    7.84Γ—104 N7.84 \times 10^{4} \, \text{N}
  • d)
    1.57Γ—105 N1.57 \times 10^{5} \, \text{N}

Answer: c)

7.84Γ—104 N7.84 \times 10^{4} \, \text{N}

Explanation:

F=Gm1β‹…m2r2=(6.67Γ—10βˆ’11)(500)(5.97Γ—1024)(1000Γ—103)2=7.84Γ—104 NF = G \frac{{m_1 \cdot m_2}}{{r^2}} = \frac{{(6.67 \times 10^{-11})(500)(5.97 \times 10^{24})}}{{(1000 \times 10^3)^2}} = 7.84 \times 10^{4} \, \text{N}

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