chapter23 part1 nadiah

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Nadiah Alenazi 1 Chapter 23 Chapter 23 Electric Fields Electric Fields 23.1 Properties of Electric 23.1 Properties of Electric Charges Charges 23.3 Coulomb’s Law 23.3 Coulomb’s Law 23.4 The Electric Field 23.4 The Electric Field 23.6 Electric Field Lines 23.6 Electric Field Lines 23.7 Motion of Charged 23.7 Motion of Charged Particles in a Uniform Particles in a Uniform Electric Field Electric Field

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  • Chapter 23
    Electric Fields

    23.1 Properties of Electric Charges

    23.3 Coulombs Law

    23.4 The Electric Field

    23.6 Electric Field Lines

    23.7 Motion of Charged Particles in a Uniform Electric Field

    Nadiah Alenazi

  • 23.1 Properties of Electric Charges

    There are two kinds of electric charges in nature:Positive Negative Like charges repel one another and Unlike charges attract one another.Electric charge is conserved.Charge is quantized q=Ne

    e = 1.6 x 10-19 C

    N is some integer

    Nadiah Alenazi

  • 23.3 Coulombs Law

    From Coulombs experiments, we can generalize the following properties of the electric force between two stationary charged particles.

    The electric force

    is inversely proportional to the square of the separation r between the particles and directed along the line joining them. is proportional to the product of the charges q1 and q2 on the two particles.is attractive if the charges are of opposite sign and repulsive if the charges have the same sign.

    Nadiah Alenazi

  • Consider two electric charges: q1 and q2The electric force F between these two charges separated by a distance r is given by Coulombs Law The constant ke is called Coulombs constant0 is the permittivity of free spaceThe smallest unit of charge e is the charge on an electron (-e) or a proton (+e) and has a magnitude e = 1.6 x 10-19 C

    Nadiah Alenazi

  • Example 23.1 The Hydrogen Atom

    The electron and proton of a hydrogen atom are separated (on the average) by a distance of approximately 5.3 x 10-11 m. Find the magnitudes of the electric force.

    Nadiah Alenazi

  • When dealing with Coulombs law, you must remember that force is a vector quantityThe law expressed in vector form for the electric force exerted by a charge q1 on a second charge q2, written F12, iswhere r is a unit vector directed from q1 toward q2The electric force exerted by q2 on q1 is equal in magnitude to the force exerted by q1 on q2 and in the opposite direction; that is, F21= -F12.

    Nadiah Alenazi

  • When more than two charges are present, the force between any pair of them is given by Equation Therefore, the resultant force on any one of them equals the vector sum of the forces exerted by the various individual charges. For example, if four charges are present, then the resultant force exerted by particles 2, 3, and 4 on particle 1 is

    Nadiah Alenazi

  • Double one of the chargesforce doublesChange sign of one of the chargesforce changes directionChange sign of both chargesforce stays the sameDouble the distance between chargesforce four times weakerDouble both chargesforce four times stronger

    Nadiah Alenazi

  • Example:

    Three point charges are aligned along the x axis as shown. Find the electric force at the charge 3nC.

    Nadiah Alenazi

  • Example 23.2 Find the Resultant Force

    Consider three point charges located at the corners of a right triangle, where q1=q3= 5.0C, q2= 2.0 C, and a= 0.10 m. Find the resultant force exerted on q3.

    Nadiah Alenazi

  • Nadiah Alenazi

  • Nadiah Alenazi

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