Current in a Current Carrying Conductor (OCR AS Physics): Revision Note

Exam code: H156

Ashika

Written by: Ashika

Reviewed by: Caroline Carroll

Updated on

Mean Drift Velocity of Charge Carriers

  • In a conductor, the current is due to the movement of charge carriers

  • The charge carriers can be negative or positive, however, the current is always taken to be in the same direction

  • In conductors, the charge carrier is usually free electrons

    • However, these electrons only travel a small difference before colliding with a metal ion

    • This means they have a relatively slow drift velocity, v

  • In the diagram below, the current in each conductor is from right to left but the charge carriers move in opposite directions shown by the direction of the drift velocity v

    • In diagram A (positive charge carriers), the drift velocity is in the same direction as the current

    • In diagram B (negative charge carriers), the drift velocity is in the opposite direction to the current

Charge carriers diagram, downloadable AS & A Level Physics revision notes

Conduction in a current-carrying conductor

 

  • The drift velocity is the average velocity of the charge carriers travelling through the conductor

    • You will find this value is relatively slow (∼ 10-3 m s-1)

  • However, since the number density of charge carriers is so large, the current flow still seems to happen instantaneously

Calculating Current in a Current Carrying Conductor

  • The current can be expressed in terms of the number density (number of charge carriers per unit volume) n, the cross-sectional area A, the drift velocity v and the charge of the charge carriers q

Current conductor equation, downloadable AS & A Level Physics revision notes

Current in a conductor equation

  • The same equation is used whether the charge carriers are positive or negative

    • The minus sign will indicate current in the opposite direction to the charge carriers

  • The charge q will be e for electrons (-1.60 × 10-19 C)

  • The number density n represents the number of free charge carriers (electrons) per unit volume

    • Conductors, such as metals, have a high value of n

    • Insulators, such as plastics, have a small value of n

  • The cross-sectional area A of a wire is the area of a circle

A = πr2

  • Where:

    • r = radius of the wire (m)

  • This equation shows:

    • v is inversely proportional to n meaning more charge carriers per unit volume will slow down their speed through the conductor

    • I is directly proportional to since greater n means greater charge is flowing and therefore a larger current I. When the value of n is lower, the charge carriers must travel faster to carry the same current

Worked Example

A copper wire has 9.2 × 1028 free electrons m-3. The wire has a current of 3.5 A and a cross-sectional area of 1.5 mm2.Calculate the average drift speed of the electrons.

Answer:

Examiner Tips and Tricks

Remember that the cross-sectional area is in m2, the drift velocity is in m s-1 and the number density is in m-3. Therefore, sometimes unit conversions from cm or mm may be required, so make sure you're comfortable with these.

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Ashika

Author: Ashika

Expertise: Physics Content Creator

Ashika graduated with a first-class Physics degree from Manchester University and, having worked as a software engineer, focused on Physics education, creating engaging content to help students across all levels. Now an experienced GCSE and A Level Physics and Maths tutor, Ashika helps to grow and improve our Physics resources.

Caroline Carroll

Reviewer: Caroline Carroll

Expertise: Head of Content Delivery

Caroline graduated from the University of Nottingham with a degree in Chemistry and Molecular Physics. She spent several years working as an Industrial Chemist in the automotive industry before retraining to teach. Caroline has over 12 years of experience teaching GCSE and A-level chemistry and physics. She is passionate about delivering high-quality resources to help students achieve their full potential.