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Kendriya Vidyalaya
Karwar
Physics Project
Class XII A
By: Atit Gaonkar
Force Due To Parallel
Current Carrying
Conductor
TOPIC
• Force Due To Parallel
Current Carrying
Conductor
Force Due To Magnetic
Field is placed in an
• When a current-carrying conductor
external magnetic field B, the magnetic force on the
conductor is given by:
• F = I (L x B)
• F = I L B sin θ
Let L1 & L2 be two current carrying conductors,
carrying current I1 & I2 separated by a
distance ‘a’ producing magnetic field B1 & B2
respectively
• Consider two parallel wires of equal length carrying
a steady current:
The two wires will exert magnetic forces on each
other.
Wire 1 will exert a magnetic force on wire 2, wire 2
will exert a magnetic force on wire 1.
• From Amperean Law we know that the magnetic
fields B1 & B2 :
• B1 = (μ * I1)/ 2Πa
• B2 = (μ * I2)/ 2Πa
• The wires are separated by distance ‘a’ and carry
currents I1 and I2 in the same direction.
• Wire 2, carrying current I2, sets up a magnetic field
B2 at the position of wire 1.
• The direction of the magnetic field B2 is known by
using Right Hand Thumb Rule and the direction is
perpendicular to the wire
• Therefore F21 = I1 (L x B2)
• As Angle Between L And B2 is 90

• So F21 = I1 L B2
• Therefore the force F21 = I1 L (μ I2) / 2Πa
• Rewriting the force per unit length :
• F/L = I1 (μ I2)/ 2Πa
• So, let F/L = F’
•
F’ = I1 (μ I2) / 2Πa
•
F’ = (μ I1 I2 ) / 2Πa
• The direction of F1 is towards the other conductor
and is determined by using the right hand rule
(fingers of right hand in direction of current I; palm
facing in the direction of B; thumb points in the
direction of Force)
• As the new force is directly proportional to I1 & I2 so
the new force of wire1 and wire2 over each other
will be same.

• The magnetic force that wire 1 exerts on wire 2
(F1 on 2) is equal in magnitude to and opposite in
direction to F1 (F2 on 1).
• Wire 1 and wire 2 will attract each other.
• Note: Parallel conductors carrying currents in the
same direction attract each other & parallel
conductors carrying currents in opposite directions
repel each other.
• So,
 Parallel wires with current flowing in the same
direction, attract each other.
 Parallel wires with current flowing in the opposite
direction, repel each other.
• Therefore
• Vector F21 = - Vector F12
• But | F21 | = | F12 |

• Therefore F’ = (μ I1 I2 ) / 2Πa
• When I1 = I2 = I Ampere , a = 1m , then
F’ = 2 * 10-7 N/m
• So,
• 1 Ampere can be defined as “When two current
carrying conductors placed at a separation of 1m,
and if they experiences a force of 2 * 10-7 N/m, then
the current through the conductors are said to be
1 Ampere.
Magnetics

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Magnetics

  • 2. Force Due To Parallel Current Carrying Conductor
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  • 10. TOPIC • Force Due To Parallel Current Carrying Conductor
  • 11. Force Due To Magnetic Field is placed in an • When a current-carrying conductor external magnetic field B, the magnetic force on the conductor is given by: • F = I (L x B) • F = I L B sin θ
  • 12. Let L1 & L2 be two current carrying conductors, carrying current I1 & I2 separated by a distance ‘a’ producing magnetic field B1 & B2 respectively
  • 13. • Consider two parallel wires of equal length carrying a steady current: The two wires will exert magnetic forces on each other. Wire 1 will exert a magnetic force on wire 2, wire 2 will exert a magnetic force on wire 1. • From Amperean Law we know that the magnetic fields B1 & B2 : • B1 = (μ * I1)/ 2Πa • B2 = (μ * I2)/ 2Πa
  • 14.
  • 15. • The wires are separated by distance ‘a’ and carry currents I1 and I2 in the same direction. • Wire 2, carrying current I2, sets up a magnetic field B2 at the position of wire 1. • The direction of the magnetic field B2 is known by using Right Hand Thumb Rule and the direction is perpendicular to the wire
  • 16. • Therefore F21 = I1 (L x B2) • As Angle Between L And B2 is 90 • So F21 = I1 L B2 • Therefore the force F21 = I1 L (μ I2) / 2Πa
  • 17. • Rewriting the force per unit length : • F/L = I1 (μ I2)/ 2Πa • So, let F/L = F’ • F’ = I1 (μ I2) / 2Πa • F’ = (μ I1 I2 ) / 2Πa • The direction of F1 is towards the other conductor and is determined by using the right hand rule (fingers of right hand in direction of current I; palm facing in the direction of B; thumb points in the direction of Force)
  • 18. • As the new force is directly proportional to I1 & I2 so the new force of wire1 and wire2 over each other will be same. • The magnetic force that wire 1 exerts on wire 2 (F1 on 2) is equal in magnitude to and opposite in direction to F1 (F2 on 1). • Wire 1 and wire 2 will attract each other.
  • 19. • Note: Parallel conductors carrying currents in the same direction attract each other & parallel conductors carrying currents in opposite directions repel each other.
  • 20. • So,  Parallel wires with current flowing in the same direction, attract each other.  Parallel wires with current flowing in the opposite direction, repel each other.
  • 21. • Therefore • Vector F21 = - Vector F12 • But | F21 | = | F12 | • Therefore F’ = (μ I1 I2 ) / 2Πa • When I1 = I2 = I Ampere , a = 1m , then F’ = 2 * 10-7 N/m
  • 22. • So, • 1 Ampere can be defined as “When two current carrying conductors placed at a separation of 1m, and if they experiences a force of 2 * 10-7 N/m, then the current through the conductors are said to be 1 Ampere.

Editor's Notes

  1. Presentations are a powerful communication medium.
  2. Presentations are a powerful communication medium.
  3. Presentations are a powerful communication medium.
  4. For more than 20 years, Duarte has developed presentations…
  5. …to launch products,
  6. …align employees,
  7. …increase company value,
  8. …and propel
  9. …global causes.
  10. Along the way we’ve discovered…