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Current flows on a metallic strip of width 'a'. It is places in a magnetic field such that B is perpendicular to the strip. What is the potential difference between top and bottom edge (the ones seperated by 'a' distance) if cross section area is 'S', current is 'I' and concentration of electrons in n.


Radhika Batra , 11 Years ago
Grade 11
anser 1 Answers
Askiitians Tutor Team

Last Activity: 5 Months ago

To find the potential difference between the top and bottom edges of a metallic strip subjected to a magnetic field, we can use the principles of electromagnetism, specifically the Hall effect. When a current-carrying conductor is placed in a magnetic field, a voltage is induced across the conductor, which is perpendicular to both the current and the magnetic field. Let's break this down step by step.

Understanding the Setup

We have a metallic strip with the following characteristics:

  • Width: 'a'
  • Cross-sectional area: 'S'
  • Current: 'I'
  • Concentration of electrons: 'n'
  • Magnetic field: 'B', which is perpendicular to the strip

Applying the Hall Effect

When the current 'I' flows through the strip, it creates a magnetic force due to the magnetic field 'B'. This force acts on the charge carriers (electrons) moving through the strip. The force can be described by the equation:

F = q(v × B)

Where:

  • F: Magnetic force on the charge carriers
  • q: Charge of the electron (approximately -1.6 x 10-19 C)
  • v: Drift velocity of the electrons
  • B: Magnetic field strength

Calculating Drift Velocity

The drift velocity 'v' of the electrons can be calculated using the formula:

v = I / (n * A * q)

Where:

  • A: Cross-sectional area 'S'

Finding the Hall Voltage

The Hall voltage (VH) induced across the width 'a' of the strip can be expressed as:

VH = B * I * (a / (n * q * S))

Here’s how we derive this:

  • The magnetic force causes a separation of charge, leading to a potential difference across the width 'a'.
  • The Hall voltage is directly proportional to the magnetic field strength 'B' and the current 'I'.
  • It is inversely proportional to the product of the charge carrier concentration 'n', the charge 'q', and the cross-sectional area 'S'.

Final Expression for Potential Difference

Thus, the potential difference between the top and bottom edges of the metallic strip can be summarized as:

VH = \frac{B \cdot I \cdot a}{n \cdot q \cdot S}

This equation gives you a clear understanding of how the potential difference arises due to the interaction of the magnetic field with the current-carrying strip. The greater the magnetic field or current, the larger the potential difference, while a higher concentration of charge carriers or larger cross-sectional area reduces it.

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