lecuture23 currentohmslaw

26
Electric Current and Resistance

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Lecture for Payap University General Science Course

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Page 1: Lecuture23 currentohmslaw

Electric Current and Resistance

Page 2: Lecuture23 currentohmslaw

Batteries and Direct Current

Electric current is the flow of electric charge, measured in units of Amperes (A)

1A = 1C/s

A battery is a source of electric energy – it converts chemical energy into electric energy.

Page 3: Lecuture23 currentohmslaw

Batteries and Direct Current

In a circuit, electrons flow from the negative electrode to the positive one.

The positive electrode is called the anode; the negative electrode is the cathode.

A battery provides a constant source of voltage – it maintains a constant potential difference between its terminals.

André-Marie Ampère (1775 – 1836) was a French physicist who discovered electromagnetism

Page 4: Lecuture23 currentohmslaw

Batteries and Direct Current

The potential difference between the battery terminals when the battery is not connected to anything is called the electromotive force, emf.

Page 5: Lecuture23 currentohmslaw

17.1 Batteries and Direct CurrentThe actual terminal voltage of the battery is always less than the emf, due to internal resistance. Usually the difference is very small.

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17.1 Batteries and Direct Current

When batteries are connected in series, the total voltage is the sum of the individual voltages.

Page 7: Lecuture23 currentohmslaw

17.1 Batteries and Direct Current

When batteries of equal voltage are connected in parallel, the total voltage does not change; each battery supplies part of the total current.

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17.1 Batteries and Direct Current

Page 9: Lecuture23 currentohmslaw

17.2 Current and Drift Velocity

Current is the time rate of flow of charge.

SI unit of current: the ampere, A.

Page 10: Lecuture23 currentohmslaw

17.2 Current and Drift Velocity

Historically, the direction of current has been taken to be from positive to negative; this is opposite to the way electrons flow. However, this seldom matters.

Page 11: Lecuture23 currentohmslaw

17.2 Current and Drift Velocity

Electrons do not flow like water in a pipe. In the absence of voltage, they move randomly at high speeds, due to their temperature.

When a voltage is applied, a very small drift velocity is added to the thermal motion, typically around 1 mm/s; this is enough to yield the observed current.

Page 12: Lecuture23 currentohmslaw

17.3 Resistance and Ohm’s LawIf there is a potential difference across a conductor, how much current flows?

The ratio between the voltage and the current is called the resistance.

SI unit of resistance: the ohm, Ω.

Page 13: Lecuture23 currentohmslaw

17.3 Resistance and Ohm’s Law

An ohmic material is one whose resistance is constant.

Page 14: Lecuture23 currentohmslaw

17.3 Resistance and Ohm’s Law

Ohm’s law is valid only for ohmic materials:

The resistance of a particular object depends on its length, cross-sectional area, material, and temperature.

Page 15: Lecuture23 currentohmslaw

17.3 Resistance and Ohm’s Law

As expected, the resistance is proportional to the length and inversely proportional to the cross-sectional area (why?):

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

Page 16: Lecuture23 currentohmslaw

17.3 Resistance and Ohm’s LawIn this table, you can easily see the differences between the resistivities of conductors, semiconductors, and insulators.

Page 17: Lecuture23 currentohmslaw

17.3 Resistance and Ohm’s Law

For many materials, the temperature dependence of the resistivity is approximately linear, as long as the temperature change is not too large.

The constant α is called the temperature coefficient of resistivity. Some values of α are listed in the table on the previous page.

Page 18: Lecuture23 currentohmslaw

17.3 Resistance and Ohm’s Law

Some materials exhibit a curious phenomenon: at a very low temperature called the critical temperature, their resistivity drops abruptly to zero.

These are called superconductors; they have a number of unique properties. They are impractical for everyday home use, however, as they must be cooled to cryogenic temperatures.

Page 19: Lecuture23 currentohmslaw

17.4 Electric Power

Power, as usual, is the rate at which work is done. For work done by electricity:

Rewriting,

For ohmic materials, we can write:

Page 20: Lecuture23 currentohmslaw

17.4 Electric Power

So, where does this power go? It is changed to heat in resistive materials.

Page 21: Lecuture23 currentohmslaw

17.4 Electric Power

Electric appliances are rated in watts, assuming standard household voltage.

Page 22: Lecuture23 currentohmslaw

17.4 Electric Power

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17.4 Electric PowerThe electric company typically bills us for kilowatt-hours (kW-h), a unit of energy.

We can reduce our energy usage by buying efficient appliances.

Page 24: Lecuture23 currentohmslaw

Review of Chapter 17

A battery produces emf; positive terminal is the anode, negative is the cathode

emf is measured in volts; it is the number of joules the battery supplies per coulomb of charge

An electric current can exist only in a complete circuit

Resistance:

Page 25: Lecuture23 currentohmslaw

Review of Chapter 17

Ohm’s law is obeyed if the resistance is constant:

The resistance of an object depends on its length, cross-sectional area, and resistivity.

Page 26: Lecuture23 currentohmslaw

Review of Chapter 17

Power is the rate at which work is done.