unit 3, day 4: microscopic view of electric current current density drift velocity speed of an...
TRANSCRIPT
Unit 3, Day 4: Microscopic View of Electric Current
• Current Density
• Drift Velocity
• Speed of an Electron in as Wire
• Electric Field inside a Current Carrying Conductor
Current Density
• When a potential difference is applied across a conducting wire, an electric field is generated parallel to the walls of the wire
• Inside the conductor, the E-field is no longer zero, because charges are free to move within the conductor
• Current Density is defined as the current through the wire per unit of Cross-Sectional Area
• If the current density is not uniform:
• The direction of j is usually in the direction of the E-Field
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Drift Velocity• When the E-Field is first applied, the electrons
initially accelerate but soon reach a more or less steady state average velocity.
• This average velocity is in the direction opposite of the E-Field and is known drift velocity
• Drift velocity is due to electrons colliding with metal atoms in the conductor
Drift Velocity Calculation
• n - Free electrons (of charge e) travel a displacement l, in a time Δt, through a cross-sectional area A, at a current density j, The drift velocity is:
• Note: the (-) sign indicates the direction of (positive - conventional) current, which is opposite to the direction of the velocity of the electrons
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Speed of an Electron in a Wire
• Given: Cu wire, Φ=3.2 mm (r = 1.6 x 10-3m) I=5.0A, T = 20°C (293 K), assuming 1 free electron per atom:
• Note: the rms velocity of thermal electrons in an ideal gas is a factor of 109 faster!
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Electric Field inside a Current Carrying Conductor
• Current carrying conductor of length l and cross-sectional area A, having resistance R, with a potential difference across it of ΔV
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