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General Physics (PHY 2140)

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General Physics (PHY 2140). Lecture 5. Electrostatics Electrical energy potential difference and electric potential potential energy of charged conductors Capacitance and capacitors. http://www.physics.wayne.edu/~apetrov/PHY2140/. Chapter 16. Lightning Review. Last lecture:

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slide1
General Physics (PHY 2140)

Lecture 5

  • Electrostatics
      • Electrical energy
        • potential difference and electric potential
        • potential energy of charged conductors
      • Capacitance and capacitors

http://www.physics.wayne.edu/~apetrov/PHY2140/

Chapter 16

lightning review
Lightning Review
  • Last lecture:
  • Flux. Gauss’s law.
    • simplifies computation of electric fields
  • Potential and potential energy
    • electrostatic force is conservative
    • potential (a scalar) can be introduced as potential energy of electrostatic field per unit charge
  • Review Problem: Perhaps you have noticed sudden gushes of rain or hail moments after lightning strokes in thunderstorms. Is there any connection between the gush and the stroke or thunder? Or is this just a coincidence?
16 2 electric potential and potential energy due to point charges
16.2 Electric potential and potential energy due to point charges
  • Electric circuits: point of zero potential is defined by grounding some point in the circuit
  • Electric potential due to a point charge at a point in space: point of zero potential is taken at an infinite distance from the charge
  • With this choice, a potential can be found as
  • Note: the potential depends only on charge of an object, q, and a distance from this object to a point in space, r.
superposition principle for potentials
Superposition principle for potentials
  • If more than one point charge is present, their electric potential can be found by applying superposition principle

The total electric potential at some point P due to several point charges is the algebraic sum of the electric potentials due to the individual charges.

  • Remember that potentials are scalar quantities!
potential energy of a system of point charges
Potential energy of a system of point charges
  • Consider a system of two particles
  • If V1 is the electric potential due to charge q1 at a point P, then work required to bring the charge q2 from infinity to P without acceleration is q2V1. If a distance between P and q1 is r, then by definition
  • Potential energy is positive if charges are of the same sign and vice versa.

q2

q1

r

P

A

mini quiz potential energy of an ion
Mini-quiz: potential energy of an ion

Three ions, Na+, Na+, and Cl-, located such, that they form corners of an equilateral triangle of side 2 nm in water. What is the electric potential energy of one of the Na+ ions?

Cl-

?

Na+

Na+

16 3 potentials and charged conductors
16.3 Potentials and charged conductors
  • Recall that work is opposite of the change in potential energy,
  • No work is required to move a charge between two points that are at the same potential. That is, W=0 if VB=VA
  • Recall:
      • all charge of the charged conductor is located on its surface
      • electric field, E, is always perpendicular to its surface, i.e. no work is done if charges are moved along the surface
  • Thus: potential is constant everywhere on the surface of a charged conductor in equilibrium

… but that’s not all!

slide8
Because the electric field is zero inside the conductor, no work is required to move charges between any two points, i.e.
  • If work is zero, any two points inside the conductor have the same potential, i.e. potential is constant everywhere inside a conductor
  • Finally, since one of the points can be arbitrarily close to the surface of the conductor, the electric potential is constant everywhere inside a conductor and equal to its value at the surface!
      • Note that the potential inside a conductor is not necessarily zero, even though the interior electric field is always zero!
the electron volt
The electron volt
  • A unit of energy commonly used in atomic, nuclear and particle physics is electron volt (eV)

The electron volt is defined as the energy that electron (or proton) gains when accelerating through a potential difference of 1 V

  • Relation to SI:

1 eV = 1.60´10-19 C·V = 1.60´10-19 J

Vab=1 V

problem solving strategy
Problem-solving strategy
  • Remember that potential is a scalar quantity
      • Superposition principle is an algebraic sum of potentials due to a system of charges
      • Signs are important
  • Just in mechanics, only changes in electric potential are significant, hence, the point you choose for zero electric potential is arbitrary.
example ionization energy of the electron in a hydrogen atom
Example : ionization energy of the electron in a hydrogen atom

In the Bohr model of a hydrogen atom, the electron, if it is in the ground state, orbits the proton at a distance of r = 5.29´10-11 m. Find the ionization energy of the atom, i.e. the energy required to remove the electron from the atom.

Note that the Bohr model, the idea of electrons as tiny balls orbiting the nucleus, is not a very good model of the atom. A better picture is one in which the electron is spread out around the nucleus in a cloud of varying density; however, the Bohr model does give the right answer for the ionization energy

slide12
In the Bohr model of a hydrogen atom, the electron, if it is in the ground state, orbits the proton at a distance of r = 5.29 x 10-11 m. Find the ionization energy, i.e. the energy required to remove the electron from the atom.

The ionization energy equals to the total energy of the electron-proton system,

Given:

r = 5.292 x 10-11 m

me = 9.11´10-31 kg

mp = 1.67´10-27 kg

|e| = 1.60´10-19 C

Find:

E=?

with

The velocity of e can be found by analyzing the force on the electron. This force is the Coulomb force; because the electron travels in a circular orbit, the acceleration will be the centripetal acceleration:

or

or

Thus, total energy is

16 4 equipotential surfaces
16.4 Equipotential surfaces
  • They are defined as a surface in space on which the potential is the same for every point (surfaces of constant voltage)
  • The electric field at every point of an equipotential surface is perpendicular to the surface
  • convenient to represent by drawing equipotential lines
16 6 the definition of capacitance
16.6 The definition of capacitance
  • Capacitor: two conductors (separated by an insulator)
    • usually oppositely charged
  • The capacitance, C, of a capacitor is defined as a ratio of the magnitude of a charge on either conductor to the magnitude of the potential difference between the conductors

a

+Q

b

-Q

slide16
A capacitor is basically two parallel conducting plates with insulating material in between. The capacitor doesn’t have to look like metal plates.
  • When a capacitor is connected to an external potential, charges flow onto the plates and create a potential difference between the plates.

Capacitor for use in high-performance audio systems.

  • Capacitors in circuits
    • symbols
    • analysis follow from conservation of energy
    • conservation of charge

-

-

-

+

units of capacitance
Units of capacitance
  • The unit of C is the farad (F), but most capacitors have values of C ranging from picofarads to microfarads (pF to F).
  • Recall, micro 10-6, nano 10-9, pico 10-12
  • If the external potential is disconnected, charges remain on the plates, so capacitors are good for storing charge (and energy).
16 7 the parallel plate capacitor
16.7 The parallel-plate capacitor
  • The capacitance of a device depends on the geometric arrangement of the conductors
  • where A is the area of one of the plates, d is the separation, e0 is a constant called the permittivity of free space,

e0= 8.85´10-12 C2/N·m2

A

+Q

d

A

-Q

problem parallel plate capacitor
Problem: parallel-plate capacitor
  • A parallel plate capacitor has plates 2.00 m2 in area, separated by a distance of 5.00 mm. A potential difference of 10,000 V is applied across the capacitor. Determine
    • the capacitance
    • the charge on each plate
slide20
A parallel plate capacitor has plates 2.00 m2 in area, separated by a distance of 5.00 mm. A potential difference of 10,000 V is applied across the capacitor. Determine
    • the capacitance
    • the charge on each plate

Solution:

Given:

DV=10,000 V

A = 2.00 m2

d = 5.00 mm

Find:

C=?

Q=?

Since we are dealing with the parallel-plate capacitor, the capacitance can be found as

Once the capacitance is known, the charge can be found from the definition of a capacitance via charge and potential difference:

16 8 combinations of capacitors
C1

C5

C3

C2

C4

16.8 Combinations of capacitors
  • It is very often that more than one capacitor is used in an electric circuit
  • We would have to learn how to compute the equivalent capacitance of certain combinations of capacitors

C2

C1

C3

a parallel combination
a

C1

+Q1

C2

+Q2

V=Vab

-Q1

-Q2

b

a. Parallel combination

Connecting a battery to the parallel combination of capacitors is equivalent to introducing the same potential difference for both capacitors,

A total charge transferred to the system from the battery is the sum of charges of the two capacitors,

By definition,

Thus, Ceq would be

parallel combination notes
Parallel combination: notes
  • Analogous formula is true for any number of capacitors,
  • It follows that the equivalent capacitance of a parallel combination of capacitors is greater than any of the individual capacitors

(parallel combination)

problem parallel combination of capacitors
Problem: parallel combination of capacitors

A 3 mF capacitor and a 6 mF capacitor are connected in parallel across an 18 V battery. Determine the equivalent capacitance and total charge deposited.

slide25
a

C1

+Q1

C2

+Q2

V=Vab

-Q1

-Q2

b

A 3 mF capacitor and a 6 mF capacitor are connected in parallel across an 18 V battery. Determine the equivalent capacitance and total charge deposited.

Given:

V = 18 V

C1= 3 mF

C2= 6 mF

Find:

Ceq=?

Q=?

First determine equivalent capacitance of C1 and C2:

Next, determine the charge

b series combination
a

+Q1

C1

-Q1

V=Vab

c

+Q2

C2

-Q2

b

b. Series combination

Connecting a battery to the serial combination of capacitors is equivalent to introducing the same charge for both capacitors,

A voltage induced in the system from the battery is the sum of potential differences across the individual capacitors,

By definition,

Thus, Ceq would be

series combination notes
Series combination: notes
  • Analogous formula is true for any number of capacitors,
  • It follows that the equivalent capacitance of a series combination of capacitors is always less than any of the individual capacitance in the combination

(series combination)

problem series combination of capacitors
Problem: series combination of capacitors

A 3 mF capacitor and a 6 mF capacitor are connected in series across an 18 V battery. Determine the equivalent capacitance.

slide29
a

+Q1

C1

-Q1

V=Vab

c

+Q2

C2

-Q2

b

A 3 mF capacitor and a 6 mF capacitor are connected in series across an 18 V battery. Determine the equivalent capacitance and total charge deposited.

Given:

V = 18 V

C1= 3 mF

C2= 6 mF

Find:

Ceq=?

Q=?

First determine equivalent capacitance of C1 and C2:

Next, determine the charge

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