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A uniform electric field is assumed to
Evaluate this integral
As we defined the electric field intensity as the force on a unit test

  charge               ,similarly we define the potential difference V as the work done

  (by an external source) in moving a unit positive test charge from one point
  to another in an electric field.




Hence the potential difference between initial point B to a final point A is
is positive if work done is positive in carrying the positive
charge from B to A.
The potential difference
For N no of charges
This equation is true for static fields, but we had to modify it for the
  Time-varying fields which we’ll stud later on.


Any field that satisfies this equation is said to be a conservative field.
For a short element of small length
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4
Emt ch 4

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Emt ch 4

  • 1.
  • 2.
  • 3.
  • 4.
  • 5.
  • 6. A uniform electric field is assumed to Evaluate this integral
  • 7.
  • 8.
  • 9.
  • 10.
  • 11.
  • 12.
  • 13.
  • 14.
  • 15.
  • 16. As we defined the electric field intensity as the force on a unit test charge ,similarly we define the potential difference V as the work done (by an external source) in moving a unit positive test charge from one point to another in an electric field. Hence the potential difference between initial point B to a final point A is
  • 17. is positive if work done is positive in carrying the positive charge from B to A.
  • 18.
  • 19.
  • 21.
  • 22.
  • 23.
  • 24.
  • 25. For N no of charges
  • 26.
  • 27.
  • 28.
  • 29. This equation is true for static fields, but we had to modify it for the Time-varying fields which we’ll stud later on. Any field that satisfies this equation is said to be a conservative field.
  • 30.
  • 31. For a short element of small length