SPHY 215 General Physics Spring 2022 Notes

Course Information

  • Instructor/Presenter: Laurence L. Henry, PhD

  • Course Description: The syllabus and course outline are posted on MOODLE in the Announcements folder. Students must read it carefully and completely.

  • Assignment Information:

    • Assignment #1 will be posted shortly.

    • Submission details are provided on MOODLE.

  • Reading Requirement: Students are instructed to read relevant references online regarding the topic of Gravitation as indicated in the Course Outline/Syllabus.

Lecture Overview: Gravitation

  • Main topics of the lecture include:

    • Concept of a gravitational field

    • Newton's law of gravitation

    • Principle of Superposition and applications to multiple point mass gravitation problems

    • Two shell theorems related to gravitation

    • Definition and explanation of conservative fields

    • Gravitational potential

    • Gravitational potential energy

Newton’s Law of Gravitation

  • Definition of Point Mass: A point mass is defined as a mass where all its mass is concentrated at a single point, or when the distances involved are large compared to the size of the masses being considered.

  • Mass Representation: Mass is symbolized as M or m and can be distinguished using subscripts (e.g., m1, m2).

  • SI Units:

    • Mass must be expressed in kilograms (kg) or their multiples.

    • Distances must be measured in meters (m).

  • Newton's Law of Gravitation: The gravitational force between two point masses is given by the formula: F=GMmr2F = \frac{GMm}{r^2}

    • Where:

    • F = Gravitational force

    • G = Gravitational constant = $6.67 \times 10^{-11} \text{N} \cdot \text{m}^2/\text{kg}^2$

    • M and m = masses of the objects

    • r = distance between the centers of the two masses.

  • Force Order of Subscripts: It’s important to note that the order of the subscripts matters, e.g.:

    • For m1 attracting m2: F<em>12=Gm</em>1m2r2F<em>{12} = \frac{G m</em>1 m_2}{r^2}

    • For m2 attracting m1: F<em>21=Gm</em>1m2r2F<em>{21} = \frac{G m</em>1 m_2}{r^2}

Example of Calculating Gravitational Force

  • Problem: Calculate the gravitational force between two masses, where m = 25.6 kg and M = 156.8 kg at a distance of r = 15.8 cm.

  • Solution: Convert cm to m: r = 0.158 m.

  • Force calculation:
    F=(6.67×1011Nm2/kg2)(156.8kg)(25.6kg)(0.158)2F = \frac{ (6.67 \times 10^{-11} \text{N} \cdot \text{m}^2/\text{kg}^2)(156.8 \text{kg})(25.6 \text{kg})}{(0.158)^2}

Principle of Superposition

  • Definition: The Principle of Superposition allows us to calculate the net force acting on a point mass due to multiple other point masses.

  • Application: The net force is the sum of the forces exerted by all other masses individually acting on the point mass.

  • Example: Refer to examples posted on Moodle in announcements regarding this principle.

    • For multiple masses:
      F<em>5=F</em>51+F<em>52+F</em>53+F<em>54+F</em>56F<em>5 = F</em>{51} + F<em>{52} + F</em>{53} + F<em>{54} + F</em>{56}

  • Assignment Connection: Problem #5 of Assignment #1 requires the use of the Principle of Superposition.

Two Shell Theorems Dealing with Gravitation

  1. Theorem #1: The gravitational force between a point mass m and mass M is given by:
    FmM=GmMr2F_{mM} = \frac{G m M}{r^2}

  2. Theorem #2: For a point mass m inside a spherical shell of mass M:
    FmM=0F_{mM} = 0

  • The implications of these theorems will vary depending on the configuration of the mass distribution.

Conservative Fields

  • Definition: A gravitational field is considered a conservative field when the work done moving between two points A and B is independent of the path taken.

  • Graphical Representation:

    • Work done in different paths from point A to point B will yield the same result:

    • W<em>path1=W</em>path2=Wpath3W<em>{path1} = W</em>{path2} = W_{path3}

Gravitational Field Strength (GFS)

  • Definition: GFS at a point in a gravitational field caused by mass M is the force acting on a test mass m placed in this field, divided by the mass of the test mass m.

  • Mathematically Expressed:
    GFS=Fm=GMm/r2m=GMr2GFS = \frac{F}{m} = \frac{GMm/r^2}{m} = \frac{GM}{r^2}

  • Units: The unit for GFS is N/kg.

  • Example of GFS:

    • At the surface of Earth:
      GFS=(6.67×1011Nm2/kg2)(5.98×1024kg)(6.37×106extm)2=9.83extN/kgGFS = \frac{(6.67 \times 10^{-11} \text{N} \cdot \text{m}^2/\text{kg}^2)(5.98 \times 10^{24} \text{kg})}{(6.37 \times 10^6 ext{m})^2} = 9.83 ext{N/kg}

    • This value represents the acceleration due to gravity (g) at the surface of the Earth.

Gravitational Potential (Vg)

  • Definition: The gravitational potential Vg at a location at a specific distance from mass M is defined as:
    Vg=GMrV_g = \frac{GM}{r}

  • Units: Measured in Joules/kg (J/kg).

  • Examples:

    • (i) Compute the gravitational potential at a distance of 6.89 m from an 8.9 kg mass:
      Vg=(6.67×1011Nm2/kg2)(8.9extkg)6.89extm=8.62×1011extJ/kgV_g = \frac{(6.67 \times 10^{-11} \text{N} \cdot \text{m}^2/\text{kg}^2)(8.9 ext{kg})}{6.89 ext{m}} = 8.62 \times 10^{-11} ext{J/kg}

Gravitational Potential Energy (Ug)

  • Definition: The gravitational potential energy U that a mass m has when located in a gravitational field created by mass M is given by: Ugravity=GMmrU_{gravity} = \frac{GMm}{r}

    • Reference: Potential energy is considered zero at infinity (when two masses are infinitely far apart).

  • Example Calculation:

    • For a mass of 1.6 kg at a distance of 6.89 m from an 8.9 kg mass:
      U=(6.67×1011Nm2/kg2)(8.9extkg)(1.6extkg)6.89extm=1.38×1010extJU = \frac{(6.67 \times 10^{-11} \text{N} \cdot \text{m}^2/\text{kg}^2)(8.9 ext{kg})(1.6 ext{kg})}{6.89 ext{m}} = 1.38 \times 10^{-10} ext{J}

Important Notes on Potential and Potential Energy

  • Reference Context: Unless a reference is provided, gravitational potential and gravitational potential energy are meaningless.

  • Default Reference: The zero of energy is assumed to be at an infinite distance from the mass causing the gravitational field.

  • Gravitational Influence: Both masses set up gravitational fields, but the examples often focus on the field present before the second mass is added.

Summary of Key Gravitation Concepts

  • Newton’s Law of Gravitation: F=GMmr2F = \frac{GMm}{r^2} (magnitude), where the force is attractive.

  • Usage of Superposition Principle: To find net gravitational force from multiple point masses.

  • Shell Theorems: Highlight behavior of gravitational fields given certain uniform mass distributions.

  • Conservative Field Nature: Work in conservative fields is path-independent.

  • Gravitational Field Strength: GFS=GMr2GFS = \frac{GM}{r^2}

  • Gravitational Potential and Energy:

    • Vg=GMrV_g = \frac{GM}{r}

    • Ug=GMmrU_g = \frac{GMm}{r}

Closing Remarks on Gravitational Physics

  • Gravitation Completion: Problems involving potential energy, example given includes:

    • What is the binding energy of the earth-moon system?
      U=GMm<em>MeR</em>emU = \frac{GMm<em>{Me}}{R</em>{em}}

The symbols used in the notes, particularly in the context of gravitation, represent various physical quantities and units:

  • F: Represents Gravitational force, measured in Newtons (N).

  • G: Denotes the Gravitational constant, with a value of 6.67×1011Nm2/kg26.67 \times 10^{-11} \text{N} \cdot \text{m}^2/\text{kg}^2.

  • M and m: Symbolize the masses of objects, typically expressed in kilograms (kg).

  • r: Represents the distance between the centers of two masses, measured in meters (m).

  • GFS: Stands for Gravitational Field Strength, with units of N/kg.

  • Vg: Represents Gravitational Potential, measured in Joules/kg (J/kg).

  • U or Ug: Denotes Gravitational Potential Energy, measured in Joules (J).

Additionally, units like kg (kilogram), m (meter), N (Newton), and J (Joule) are used for mass, distance, force, and energy, respectively.