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Chapter 17

Chapter 17. Current and Resistance. Electric Current. Whenever electric charges of like signs move, an electric current is said to exist The current is the rate at which the charge flows through this surface Look at the charges flowing perpendicularly to a surface of area A

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Chapter 17

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  1. Chapter 17 Current and Resistance

  2. Electric Current • Whenever electric charges of like signs move, an electric current is said to exist • The current is the rate at which the charge flows through this surface • Look at the charges flowing perpendicularly to a surface of area A • The SI unit of current is Ampere (A) • 1 A = 1 C/s

  3. Example 17.1 – Page 571 • The amount of charge that passes through the filament of a certain lightbulb in 2.0 s is 1.67 C. Find • A) the current in the bulb, and • B) the number of electrons that pass through the filament in 5 s.

  4. Electric Current, cont • The direction of the current is the direction positive charge would flow • This is known as conventional current direction • In a common conductor, such as copper, the current is due to the motion of the negatively charged electrons • It is common to refer to a moving charge as a mobile charge carrier • A charge carrier can be positive or negative

  5. Current and Drift Speed • Charged particles move through a conductor of cross-sectional area A • n is the number of charge carriers per unit volume • n A Δx is the total number of charge carriers

  6. Current and Drift Speed, cont • The total charge is the number of carriers times the charge per carrier, q • ΔQ = (n A Δx) q • The drift speed, vd, is the speed at which the carriers move • vd = Δx/ Δt • Rewritten: ΔQ = (n A vd Δt) q • Finally, current, I = ΔQ/Δt = nqvdA

  7. Current and Drift Speed, final • If the conductor is isolated, the electrons undergo random motion • When an electric field is set up in the conductor, it creates an electric force on the electrons and hence a current

  8. Example 17.2 – Page 573 • A copper wire of cross-sectional area 3x10-6m2 carries a current of 10A. • A) assuming that each copper atom contributes one free electron to the metal, find the drift speed of the electrons in this wire. • B) use the ideal gas model to compare the drift speed with the random rms speed an electron would have at 200C. The density of copper is 8.92g/cm3, and its atomic mass is 63.5u.

  9. A) Need to find n=number of free charge carriers per unit volume -> 1 mole Cu contains 6.02x1023 atoms (Avogadro’s Number) -> one Cu atom contributes with 1 charge carrier to the metal -> atomic mass = #grams in a mole of substance = 63.5g -> density=mass/volume  volume = mass/density=63.5g/8.92gcm-3=7.12cm3 -> n = (#electrons/mole)/(volume/mole)

  10. B) Root mean square speed at T=20 C is ? Ideal gas model: Where: -> k = Boltzman’s constant=1.38066x10-23J/K -> T = 293 K -> me=9.11x10-31 Kg

  11. Charge Carrier Motion in a Conductor • The zig-zag black line represents the motion of charge carrier in a conductor • The net drift speed is small • The sharp changes in direction are due to collisions • The net motion of electrons is opposite the direction of the electric field

  12. Electrons in a Circuit • The drift speed is much smaller than the average speed between collisions • When a circuit is completed, the electric field travels with a speed close to the speed of light

  13. Meters in a Circuit – Ammeter • An ammeter is used to measure current • In line with the bulb, all the charge passing through the bulb also must pass through the meter

  14. Meters in a Circuit – Voltmeter • A voltmeter is used to measure voltage (potential difference) • Connects to the two ends of the bulb

  15. Resistance • In a conductor, the voltage applied across the ends of the conductor is proportional to the current through the conductor • The constant of proportionality is the resistance of the conductor

  16. Resistance, cont • Units of resistance are ohms (Ω) • 1 Ω = 1 V / A • Resistance in a circuit arises due to collisions between the electrons carrying the current with the fixed atoms inside the conductor

  17. Georg Simon Ohm (German Physicist)(1787-1854) “As a high school teacher, Ohm started his research with the electrochemical cell, invented by Italian Count Alessandro Volta. Using equipment of his own creation, Ohm determined that there is a direct proportionality between the potential difference (voltage) applied across a conductor and the resultant electric current which flows through it – which we now know as Ohm's law. Using the results of his experiments, Ohm was able to define the fundamental relationship among voltage, current, and resistance, which represents the true beginning of electrical circuit analysis.”

  18. Ohm’s Law • Experiments show that for many materials, including most metals, the resistance remains constant over a wide range of applied voltages or currents • This statement has become known as Ohm’s Law • ΔV = I R • Ohm’s Law is an empirical relationship that is valid only for certain materials • Materials that obey Ohm’s Law are said to be ohmic

  19. Ohm’s Law, cont • An ohmic device • The resistance is constant over a wide range of voltages • The relationship between current and voltage is linear • The slope is related to the resistance

  20. Ohm’s Law, final • Non-ohmic materials are those whose resistance changes with voltage or current • The current-voltage relationship is nonlinear • A diode is a common example of a non-ohmic device

  21. Resistivity • The resistance of an ohmic conductor is proportional to its length, L, and inversely proportional to its cross-sectional area, A • ρ is the constant of proportionality and is called the resistivity of the material • See table 17.1, page 577

  22. Example 17.3 – Page 578 • A) Calculate the resistance per unit length of a 22-gauge nichrome wire of radius 0.321mm. • B) If a potential difference of 10V is maintained across a 1m length of the nichrome wire, what is the current in the wire? • C) The wire is melted down and recast with twice its original length. Find the new resistance RN as a multiple of the old resistance R0.

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