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Chapter 19 A Microscopic View of Electric Circuits
23

Chapter 19

Feb 23, 2016

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Chapter 19. A Microscopic View of Electric Circuits. Current in a Circuit. A microscopic view of electric circuits: Are charges used up in a circuit? How is it possible to create and maintain a nonzero electric field inside a wire? What is the role of the battery in a circuit?. - PowerPoint PPT Presentation
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Page 1: Chapter 19

Chapter 19

A Microscopic View of Electric Circuits

Page 2: Chapter 19

Steady state and static equilibrium

Static equilibrium: • no charges are moving

Steady state (Dynamic Equilibrium): • charges are moving• their velocities at any location do not change with time• no change in the deposits of excess charge anywhere

Current in a Circuit

In an electric circuit the system does not reach equilibrium!

A microscopic view of electric circuits:• Are charges used up in a circuit?• How is it possible to create and maintain a nonzero electric

field inside a wire?• What is the role of the battery in a circuit?

Page 3: Chapter 19

IB = IA in a steady state circuit

What is used up in the light bulb?We cannot get something for nothing!

Energy is transformed from one form to another

Electric field – accelerates electronFriction – energy is lost to heatBattery – chemical energy is used up

Closed circuit – energy losses to heat:not an isolated system!

Current in Different Parts of a Circuit

Page 4: Chapter 19

Momentum principle:

E

Speed of the electron:

Average ‘drift’ speed: - average time betweencollisions

The Drude Model

Page 5: Chapter 19

Average ‘drift’ speed: - average time betweencollisions

For constant temperature

u – mobility of an electron

Electron current:

The Drude Model

Paul Drude(1863 - 1906)

Page 6: Chapter 19

In steady state current is the same everywhere in a series circuit.

ii

What is the drift speed?

Note: density of electrons n cannot change if same metal

What is E?

EthickEthin

E and Drift Speed

Page 7: Chapter 19

2 mm1 mm

1.5.n1 = n2

2.u1 = u2

Every second 1018 electrons enter the thick wire. How many electrons exit from the thin wire every second?

1018

Question

A) 1018

B) 1.5 x 1018

C) 2 x 1018

D) 4 x 1018

E) 12 x 1018

Page 8: Chapter 19

2 mm1 mm

1.5.n1 = n2

2.u1 = u2

What is the ratio of the electric field, E1/E2?

1018

Question

A) 3:1B) 6:1C) 8:1D) 12:1

Page 9: Chapter 19

Does current fill the wire? Is E uniform across the wire?

E must be parallel to the wire

E is the same along the wire

0 0VAB VCD

Direction of Electric Field in a Wire

Page 10: Chapter 19

Connecting a Circuit

The initial transient

When making the final connection in a circuit, feedback forces a rapid rearrangement of the surface charges leading to the steady state.

This period of adjustment before establishing the steady state is called the initial transient.

Page 11: Chapter 19

1. Static equilibrium: nothing moving(no current)

3. Steady state: constant current (nonzero)

2. Initial transient: short-time processleading to the steady state

Connecting a Circuit

Page 12: Chapter 19

The current node rule(Kirchhoff node or junction rule [law #1]):

In the steady state, the electron current entering a node in a circuit is equal to the electron current leaving that node

(consequence of conservation of charge)

i1 = i2

i2 = i3 + i4

Current at a Node

Gustav Robert Kirchhoff (1824 - 1887)

Page 13: Chapter 19

I1 + I4 = I2 + I3

I2 = I1 + I4 - I3 = 3A

I1 + I4 = I2 + I3

I2 = I1 + I4 - I3 = -2A

1ACharge conservation:

Ii > 0 for incomingIi < 0 for outgoing

ExerciseWrite the node equation for this circuit. What is the value of I2?

What is the value of I2 if I4 is 1A?

Page 14: Chapter 19

Energy conservation (the Kirchhoff loop rule [2nd law]):

V1 + V2 + V3 + … = 0 along any closed path in a circuit

Vwire = ELVbattery = ?

V= U/q energy per unit charge

Energy in a Circuit

Page 15: Chapter 19

non-Coulomb force on each e

EC

FC

1. FC =eEC

Coulomb force on each e

2. FC =FNC

The function of a battery is to produce and maintain a charge separation.

Energy input per unit chargeemf – electromotive force

The emf is measured in Volts, but it is not a potential difference!The emf is the energy input per unit charge.

chemical, nuclear, gravitational…

Potential Difference Across the Battery

Fully charged battery.

Page 16: Chapter 19

Round-trip potential difference:

Field and Current in a Simple Circuit

We will neglect the battery’s internal resistance for the time being.

Page 17: Chapter 19

Round-trip potential difference:

Path 1

Path 2

Field and Current in a Simple Circuit

Page 18: Chapter 19

The number or length of the connecting wires has little effect on the amount of current in the circuit.

uwires >> ufilament

Work done by a battery goes mostly into energy dissipation in the bulb (heat).

V Across Connecting Wires

Page 19: Chapter 19

Nichrome wire (resistive)

Twice the Length

Current is halved when increasing the length of the wire by a factor of 2.

Page 20: Chapter 19

Doubling the Cross-Sectional Area

Nichrome wire

Electron current in the wire increases by a factor of two if the cross-sectional area of the wire doubles.

Loop: emf - EL = 0

𝑖=𝑛𝐴𝑢𝐸

Page 21: Chapter 19

Two Identical Light Bulbs in Series

Identical light bulbs

Two identical light bulbs in series are the same as one light bulb with twice as long a filament.

The filament lengths add …

Page 22: Chapter 19

1. Path ABDFA:

2. Path ACDFA:

3. Path ABDCA:

iB = iC

ibatt = 2iB

F

Two Light Bulbs in Parallel

We can think of the two bulbs in parallel as equivalent to increasing the cross-sectional area of one of the bulb filaments.

L … length of bulb filament

The filament areas add …

Page 23: Chapter 19

The current node rule (Charge conservation)Kirchhoff node or junction rule [1st law]:In the steady state, the electron current entering a node in a circuit is equal to the electron current leaving that node

Analysis of Circuits

V1 + V2 + V3 + … = 0 along any closed path in a circuit

The loop rule (Energy conservation)Kirchhoff loop rule [2nd law]:

V= U/q energy per unit charge

Electron current: i = nAuE Conventional current: I = |q|nAuE