lecture23 ohmslaw

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Electric Current and Resistance

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Lecture for General Science Course Payap

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Page 1: Lecture23 ohmslaw

Electric Current and Resistance

Page 2: Lecture23 ohmslaw

Batteries and Direct Current

Electric current is the flow of electric charge, usually denoted by the symbol I

It is 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: Lecture23 ohmslaw

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: Lecture23 ohmslaw

Batteries and direct current

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

Resistor

Page 5: Lecture23 ohmslaw

Some symbols for circuit diagrams

Page 6: Lecture23 ohmslaw

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 7: Lecture23 ohmslaw

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.

Page 8: Lecture23 ohmslaw

Batteries and Direct Current

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

Page 9: Lecture23 ohmslaw

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.

Page 10: Lecture23 ohmslaw

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 a large observed current.

Page 11: Lecture23 ohmslaw

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 12: Lecture23 ohmslaw

Resistance and Ohm’s Law

An ohmic material is one whose resistance is constant.

Page 13: Lecture23 ohmslaw

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 14: Lecture23 ohmslaw

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 15: Lecture23 ohmslaw

Resistance and Ohm’s LawBig differences between the resistivities of conductors, semiconductors, and insulators.

Page 16: Lecture23 ohmslaw

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. Hot conductors don’t conduct so well.

Page 17: Lecture23 ohmslaw

Superconductors

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, because they must be cooled to cryogenic temperatures.

But they are very useful for large power transmission lines, electric rail installations,…

Page 18: Lecture23 ohmslaw

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 19: Lecture23 ohmslaw

Electric Power

Where does this power go? It is changed to heat in resistive materials.

Page 20: Lecture23 ohmslaw

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

The 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 21: Lecture23 ohmslaw

Electric Power

Page 22: Lecture23 ohmslaw

Review for today• 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:

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

Page 23: Lecture23 ohmslaw

Review for today

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

Power is the rate at which work is done. When dealing with a resistor in a circuit: