Electric Currents and Resistance

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Electric Currents and Resistance

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Electric Currents and Resistance. The Electric Battery Electric Current Ohm’s Law: Resistance and Resistors Resistivity Electric Power Microscopic View of Electric Current: Current Density and Drift Velocity. - PowerPoint PPT Presentation

Transcript of Electric Currents and Resistance

Page 1: Electric Currents and Resistance

Electric Currents and Resistance

Page 2: Electric Currents and Resistance

• The Electric Battery

• Electric Current

• Ohm’s Law: Resistance and Resistors

• Resistivity

• Electric Power

•Microscopic View of Electric Current: Current Density and Drift Velocity

Page 3: Electric Currents and Resistance

Volta discovered that electricity could be created if dissimilar metals were connected by a conductive solution called an electrolyte.

This is a simple electric cell.

Page 4: Electric Currents and Resistance

A battery transforms chemical energy into electrical energy.

Chemical reactions within the cell create a potential difference between the terminals by slowly dissolving them. This potential difference can be maintained even if a current is kept flowing, until one or the other terminal is completely dissolved.

The Electric Battery

Page 5: Electric Currents and Resistance

Several cells connected together make a battery, although now we refer to a single cell as a battery as well.

The Electric Battery

Page 6: Electric Currents and Resistance

Electric current is the rate of flow of charge through a conductor:

Unit of electric current: the ampere, A:

1 A = 1 C/s.

Electric Current

The instantaneous current is given by:

Page 7: Electric Currents and Resistance

A complete circuit is one where current can flow all the way around. Note that the schematic drawing doesn’t look much like the physical circuit!

Electric Current

Page 8: Electric Currents and Resistance

Electric CurrentCurrent is flow of charge.

A steady current of 2.5 A exists in a wire for 4.0 min. (a) How much total charge passed by a given point in the circuit during those 4.0 min? (b) How many electrons would this be?

Page 9: Electric Currents and Resistance

Electrons in a conductor have large, random speeds just due to their temperature. When a potential difference is applied, the electrons also acquire an average drift velocity, which is generally considerably smaller than the thermal velocity.

Current Density and Drift Velocity

Page 10: Electric Currents and Resistance

Current Density and Drift Velocity

We define the current density (current per unit area) – this is a convenient concept for relating the microscopic motions of electrons to the macroscopic current:

If the current is not uniform:

.

Page 11: Electric Currents and Resistance
Page 12: Electric Currents and Resistance

Charges move with a drift velocity along the wire.

Current Density and Drift Velocity

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d/ vt Total charge within the volume:

Time taken to pass through:

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Page 13: Electric Currents and Resistance

Electric Current

How to connect a battery.

What is wrong with each of the schemes shown for lighting a flashlight bulb with a flashlight battery and a single wire?

Page 14: Electric Currents and Resistance

By convention, current is defined as flowing from + to -. Electrons actually flow in the opposite direction, but not all currents consist of electrons.

Electric Current

Page 15: Electric Currents and Resistance

Experimentally, it is found that the current in a wire is proportional to the potential difference between its ends:

Ohm’s Law

Page 16: Electric Currents and Resistance

The ratio of voltage to current is called the resistance:

Ohm’s Law: Resistance and Resistors

Page 17: Electric Currents and Resistance

In many conductors, the resistance is independent of the voltage; this relationship is called Ohm’s law. Materials that do not follow Ohm’s law are called nonohmic.

Unit of resistance: the ohm, Ω:

1 Ω = 1 V/A.

Ohm’s Law

Page 18: Electric Currents and Resistance

Ohm’s Law

Current and potential.

Current I enters a resistor R as shown. (a) Is the potential higher at point A or at point B? (b) Is the current greater at point A or at point B?

Page 19: Electric Currents and Resistance

Ohm’s LawFlashlight bulb resistance.

A small flashlight bulb draws 300 mA from its 1.5-V battery. (a) What is the resistance of the bulb? (b) If the battery becomes weak and the voltage drops to 1.2 V, how would the current change?

Page 20: Electric Currents and Resistance

Standard resistors are manufactured for use in electric circuits; they are color-coded to indicate their value and precision.

Ohm’s Law

Page 21: Electric Currents and Resistance

Ohm’s LawThis is the standard resistor color code. Note that the colors from red to violet are in the order they appear in a rainbow.

Page 22: Electric Currents and Resistance

Some clarifications:

• Batteries maintain a (nearly) constant potential difference; the current varies.

• Resistance is a property of a material or device.

• Current is not a vector but it does have a direction.

• Current and charge do not get used up. Whatever charge goes in one end of a circuit comes out the other end.

Ohm’s Law

Page 23: Electric Currents and Resistance

The resistance of a wire is directly proportional to its length and inversely proportional to its cross-sectional area:

The constant ρ, the resistivity, is characteristic of the material.

Resistivity

Geometric property

Page 24: Electric Currents and Resistance

ResistivityThis table gives the resistivity and temperature coefficients of typical conductors, semiconductors, and insulators.

Page 25: Electric Currents and Resistance

Current Density and Drift Velocity

The electric field inside a current-carrying wire can be found from the relationship between the current, voltage, and resistance. Writing R = ρ l/A, I = jA, and V = El , and substituting in Ohm’s law gives:

Page 26: Electric Currents and Resistance

Power, as in kinematics, is the energy transformed by a device per unit time:

Electric Power

or

Page 27: Electric Currents and Resistance

The unit of power is the watt, W.

For ohmic devices, we can make the substitutions:

Electric Power

Page 28: Electric Currents and Resistance

Electric PowerHeadlights.

Calculate the resistance of a 40-W automobile headlight designed for 12 V.

.6.3

W40

V12 222

P

VR

R

VIVP

Page 29: Electric Currents and Resistance

What you pay for on your electric bill is not power, but energy – the power consumption multiplied by the time.

We have been measuring energy in joules, but the electric company measures it in kilowatt-hours, kWh:

1 kWh = (1000 W)(3600 s) = 3.60 x 106 J.

Electric Power

Page 30: Electric Currents and Resistance

Electric PowerElectric heater.

An electric heater draws a steady 15.0 A on a 120-V line. How much power does it require and how much does it cost per month (30 days) if it operates 3.0 h per day and the electric company charges 9.2 cents per kWh?

dollar15cent1490cent2.9162cost

kWh,162day303.0h/dayW1800

W,1800V120A15

IVP

Page 31: Electric Currents and Resistance

Electric PowerLightning bolt.

Lightning is a spectacular example of electric current in a natural phenomenon. There is much variability to lightning bolts, but a typical event can transfer 109 J of energy across a potential difference of perhaps 5 x 107 V during a time interval of about 0.2 s. Use this information to estimate (a) the total amount of charge transferred between cloud and ground, (b) the current in the lightning bolt, and (c) the average power delivered over the 0.2 s.

Page 32: Electric Currents and Resistance

• A battery is a source of constant potential difference.

• Electric current is the rate of flow of electric charge.

• Conventional current is in the direction that positive charge would flow.

• Resistance is the ratio of voltage to current:

Summary

Page 33: Electric Currents and Resistance

• Ohmic materials have constant resistance, independent of voltage.

• Resistance is determined by shape and material:

• ρ is the resistivity.

Summary

Page 34: Electric Currents and Resistance

• Power in an electric circuit:

• Direct current is constant.

• Relation between drift speed and current:

Summary

Page 35: Electric Currents and Resistance

DC Circuits

Page 36: Electric Currents and Resistance

• EMF and Terminal Voltage

• Resistors in Series and in Parallel

• Kirchhoff’s Rules

Page 37: Electric Currents and Resistance

Electric circuit needs battery or generator to produce current – these are called sources of emf (Electromotive force).

Battery is a nearly constant voltage source, but does have a small internal resistance, which reduces the actual voltage from the ideal emf:

EMF and Terminal Voltage

Terminal Voltage emf

Page 38: Electric Currents and Resistance

This resistance behaves as though it were in series with the emf.

EMF and Terminal Voltage

Page 39: Electric Currents and Resistance
Page 40: Electric Currents and Resistance

EMF and Terminal VoltageBattery with internal resistance.

A 65.0-Ω resistor is connected to

the terminals of a battery whose emf is 12.0 V and whose internal resistance is 0.5 Ω. Calculate (a) the current in the circuit, (b) the terminal voltage of the battery, Vab, and (c) the power dissipated in the resistor R and in the battery’s internal resistance r.

Page 41: Electric Currents and Resistance

A series connection has a single path from the battery, through each circuit element in turn, then back to the battery.

Resistors in Series

Page 42: Electric Currents and Resistance

•The current through each resistor is the same

•The voltage depends on the resistance.

•The sum of the voltage drops across the resistors equals the battery voltage:

Resistors in Series

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Page 43: Electric Currents and Resistance

A parallel connection splits the current; the voltage across each resistor is the same:

Resistors in Parallel

Page 44: Electric Currents and Resistance

The total current is the sum of the currents across each resistor:

Resistors in Parallel

,

The voltage across each resistor is the same:

VVVV 321

Page 45: Electric Currents and Resistance

This gives the reciprocal of the equivalent resistance:

Resistors in Parallel

Page 46: Electric Currents and Resistance

ResistorsSeries or parallel?

(a) The lightbulbs in the figure are identical. Which configuration produces more light? (b) Which way do you think the headlights of a car are wired? Ignore change of filament resistance R with current.

Page 47: Electric Currents and Resistance

ResistorsAn illuminating surprise.

A 100-W, 120-V lightbulb and a 60-W, 120-V lightbulb are connected in two different ways as shown. In each case, which bulb glows more brightly? Ignore change of filament resistance with current (and temperature).

Page 48: Electric Currents and Resistance

ResistorsCircuit with series and parallel resistors.

How much current is drawn from the battery shown? What is the current through each of the resistor?

Page 49: Electric Currents and Resistance

Resistors in Series and in Parallel

Bulb brightness in a circuit.

The circuit shown has three identical lightbulbs, each of resistance R. (a) When switch S is closed, how will the brightness of bulbs A and B compare with that of bulb C? (b) What happens when switch S is opened? Use a minimum of mathematics in your answers.

Page 50: Electric Currents and Resistance

Resistors

Analyzing a circuit.

A 9.0-V battery whose internal resistance r is 0.50 Ω is connected in the circuit shown. (a) How much current is drawn from the battery? (b) What is the terminal voltage of the battery? (c) What is the current in the 6.0-Ω resistor?

a b

c d

Page 51: Electric Currents and Resistance

Some circuits cannot be broken down into series and parallel connections. For these circuits we use Kirchhoff’s rules.

Kirchhoff’s Rules

Page 52: Electric Currents and Resistance

Junction rule: The sum of currents entering a junction equals the sum of the currents leaving it.

Kirchhoff’s Rules

Page 53: Electric Currents and Resistance

Loop rule: The sum of the changes in potential around a closed loop is zero.

Kirchhoff’s Rules

Page 54: Electric Currents and Resistance

Kirchhoff’s Rules• Junction rule:

• Loop rule:

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Page 55: Electric Currents and Resistance

1. Label each current, including its direction.

2. Identify unknowns.

3. Apply junction and loop rules; you will need as many independent equations as there are unknowns.

4.Solve the equations, being careful with signs. If the solution for a current is negative, that current is in the opposite direction from the one you have chosen.

Kirchhoff’s Rules

Page 56: Electric Currents and Resistance

Kirchhoff’s RulesUsing Kirchhoff’s rules.

Calculate the currents I1, I2, and I3 in the three branches of the circuit in the figure.

Page 57: Electric Currents and Resistance

Calculate the equivalentresistance:

Page 58: Electric Currents and Resistance

I1

I2

I

I1-I2

I

I-I1

I-I2

Page 59: Electric Currents and Resistance

Solution:

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Solving the coupled equations and express I1 and I2 in terms of I, R1, R2 and R3

Page 60: Electric Currents and Resistance

Solution:

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Page 61: Electric Currents and Resistance

• A source of emf transforms energy from some other form to electrical energy.

• A battery is a source of emf in parallel with an internal resistance.

• Resistors in series:

Summary

Page 62: Electric Currents and Resistance

• Resistors in parallel:

• Kirchhoff’s rules:

1.Sum of currents entering a junction equals sum of currents leaving it.

2.Total potential difference around closed loop is zero.

Summary

Page 63: Electric Currents and Resistance

• RC circuit has a characteristic time constant:

•Ammeter: measures current.

• Voltmeter: measures voltage.

Summary