Electrostatics Notes

Charging by Conduction

  • To charge an electroscope by conduction, a charged metal rod touches the electroscope's knob.
  • Bringing a negatively charged rod near a negatively charged electroscope causes the leaves to spread apart farther.
  • Bringing a positively charged rod near a negatively charged electroscope causes the leaves to fall closer together.

Coulomb's Law

  • Coulomb (1770s) studied the force of repulsion between charged spheres.
    • The magnitude of the force (FF) varies inversely with the square of the distance (rr) between the centers of the spheres: F1r2F \propto \frac{1}{r^2}.
    • The force varies directly with the charge of the bodies (q<em>Aq<em>A and q</em>Bq</em>B): Fq<em>Aq</em>BF \propto q<em>A q</em>B.
    • Combining these proportionalities:
      Fq<em>Aq</em>Br2F \propto \frac{q<em>A q</em>B}{r^2}
  • Coulomb's Law states that the force between two charges is equal to a constant (KK) times the product of the two charges divided by the square of the distance between them: F=Kq<em>Aq</em>Br2F = K \frac{q<em>A q</em>B}{r^2}
    • When charges are measured in Coulombs, distance in meters, and force in Newtons, the constant KK is approximately 9.0×109Nm2C29.0 \times 10^9 \frac{N \cdot m^2}{C^2}.
    • Coulomb's Law is valid only for uniform charges.

Electroscope

  • An electroscope consists of a metal knob connected by a metal stem to two thin, lightweight pieces of metal called leaves, enclosed to eliminate air currents.
  • The metal foil leaves on a neutral electroscope hang loosely together.

Vocabulary

  • Electrostatics: The study of electric charges that can be collected and held in one place.
  • Neutral: When the amount of negative charge in an object is equal to its positive charge.
  • Insulator: A material in which charge doesn't move through easily.
  • Conductor: A material that allows charges to move about easily.
  • Electroscope: A device used to measure charge, consisting of a metal knob connected by a metal stem to two thin, lightweight pieces of metal leaves, enclosed to eliminate air currents.
  • Charging by Conduction: Charging a neutral object by touching it with a charged object.
  • Charging by Induction: Charging a neutral object by bringing a charged object near it.
  • Grounding: The process of removing excess charge by connecting an object to the Earth.
  • Coulomb's Law: The magnitude of the force between point charge q<em>Aq<em>A and point charge q</em>Bq</em>B, separated by distance rr, is proportional to the product of the magnitudes of the charges and inversely proportional to the square of the distance between them.
  • Coulomb: The SI unit for charge, equivalent to the charge of 6.24×10186.24 \times 10^{18} protons or electrons.
  • Elementary Charge: The magnitude of the charge of a single electron or proton (1.602×1019C1.602 \times 10^{-19} C).

Materials and Charge

  • Ben Franklin (1750s) noted that materials have varying degrees of ability to acquire charge.
    • Hard rubber and plastic tend to become negatively charged.
    • Glass and wool tend to become positively charged.
  • Metal is a good conductor because electrons can move freely in it.
  • Plasma and graphite are also good conductors.

Electric Field Lines

  • Single Charge: For a single charge, the electric field lines radiate from that charge.
    • Field lines radiate outward from a positive charge.
    • Field lines radiate inward toward a negative charge.
    • The direction of the electric field (EE) at any point is tangent to the field line.
  • Two Equal and Unlike Charges: The electric field lines of two equal and unlike charges form continuous lines from the positive charge to the negative charge.
    • The vector at point P shows the direction of the electric field (EE) at point P.
    • Where the lines are closest, a charged particle would experience the most force.
  • Two Like Charges: The electric field lines around two like charges never connect with each other.
    • The vector at point P shows the direction of the electric field (EE) at point P.
    • A charge would experience no electrostatic force in the center where there are no electric field lines.

Calculating Electric Field

  • If and only if the charge qq' is a point charge or a uniformly charged sphere, you can calculate its electric field from Coulomb's Law:
    E=Fonqq=Kqqr2×1q=Kqr2E = \frac{F_{on q'}}{q'} = \frac{Kq q'}{r^2} \times \frac{1}{q'} = \frac{Kq}{r^2}
  • The magnitude of the force depends on the magnitude of the electric field (EE) and the magnitude of the charge (qq):
    F=EqF = Eq
  • An electric field is stronger where lines are closer together and weaker where lines are spaced out.

Vocabulary

  • Electric Field: A property of the space around a charged object that exerts force on other charged objects.
  • Electric Field Line: Indicates the direction of the force due to the electric field on a positive test charge.

Electric Field Measurement

  • The strength of an electric field is equal to the force on a positive test charge divided by the strength of the test charge:
    E=FonqqE = \frac{F_{on q'}}{q'}
  • The magnitude of the electric field is measured in Newtons per Coulomb (N/C).

Electric Potential Inside Conductors

  • When charged, the electric potential difference between any two points inside a closed metal container is zero.
  • The electric field outside the container is not zero; it is always perpendicular to the surface of the conductor.

Capacitors

  • Manufacturers make capacitors from two conducting plates separated by a thin layer of insulator.
  • These are often rolled into cylinders.
  • Engineers design different capacitors to have specific capacitances.
  • Capacitance: The ratio of the magnitude of the net charge on one plate of the capacitor to the potential difference across the plates.
    C=qVC = \frac{q}{V}
  • Capacitance is measured in farads (F), where 1 F = 1 C/V.

Charge Distribution

  • Irregular Surface: On an irregular conducting surface, the charges are closest together at sharp points.
  • Hollow Sphere: The charges on the hollow sphere are entirely on the outer surface.
  • Conducting Sphere: On a conducting sphere, the charge is evenly distributed around the surface.

Electric Potential Difference in a Uniform Field

  • Electric Potential Difference in a Uniform field: ΔV=Ed\Delta V = Ed
    • The potential difference between two locations in a uniform electric field equals the product of the electric field intensity and the distance between the locations parallel to the direction of the field.

Electric Potential

  • The electric potential difference from point A to point B:
    ΔV=V<em>BV</em>A\Delta V = V<em>B - V</em>A
  • Electric potential differences are measured with a voltmeter.
  • Electric potential difference is sometimes called voltage (do not confuse with Volts (V)).
  • Positive Electric Potential Difference:
    PE(A)+Wonchargebyyou=PE(B)PE(A) + W_{on charge}^{by you} = PE(B)
  • Negative Electric Potential Difference:
    PE(B)+Wonchargebycharge=PE(A)PE(B) + W_{on charge}^{by charge} = PE(A)

Vocabulary

  • Electric Potential Difference: The work (WonqW_{on q'}) needed to move a positive test charge from one point to another, divided by the magnitude of the test charge.
  • Volt: One joule per one Coulomb.
  • Equipotential: When the electric potential difference between two or more positions is zero.
  • Capacitor: Modern device for storing electrical energy.
  • Capacitance: The slope of the line in a charge vs. potential difference graph.

Electric Fields and Potential Energy

  • Both the gravitational force (F<em>gF<em>g) and the gravitational field (g=F</em>gmg = \frac{F</em>g}{m}) point toward Earth.
  • If you do work on a ball to lift it away from Earth's surface, the gravitational potential energy in the ball-Earth system increases.
  • The same is true for the electric field. The work done to move a charged particle in an electric field can result in the particle gaining electrical potential energy or kinetic energy, or both.
  • This is basically the same with two unlike charges: doing work to separate the charges increases the electrical potential energy of the system.
  • The longer the charge or distance moved, the greater the increase in electric potential energy (ΔPE\Delta PE).
  • To find the work done to move a charge, use the equation:

Resistance

R=ΔVIR = \frac{\Delta V}{I}

  • Measured in ohms (Ω\Omega), one ohm is the electric charge of 1 Ampere being permitted to flow when a potential difference of 1 Volt is applied across the resistance.