Kirchhoff’s loop rule Part-1

๐Ÿ”„ Loop Rule


โญ The sum of potential changes in a closed loop is always zero.

โœ…โˆ‘V=0\sum V = 0


๐Ÿ’ก Reason

โœ๏ธ Electric field is a conservative field.

In a conservative field, the work done (W) in moving a charge around a closed loop is zero.

Therefore,

W=0W = 0

Wq=0\frac{W}{q} = 0

V=0V = 0


๐ŸŽฏ Conclusion

โœ… Since the electric field is conservative, the net work done around a closed path is zero.

โœ… Hence, the algebraic sum of all potential rises and potential drops in a closed loop is zero.โˆ‘V=0\sum V = 0

๐Ÿ’ก This statement is known as Kirchhoff’s Loop Rule or Kirchhoff’s Voltage Law (KVL). ๐Ÿ”„โšก

โšก How to Calculate Potential Changes?


1๏ธโƒฃ Resistance

๐Ÿ”Œ Given

  • Resistance: R = 3 ฮฉ
  • Current: I = 2 A

๐Ÿ“Œ Rule

โžก๏ธ Along the direction of current, potential is negative (โˆ’ve).

โžก๏ธ Opposite to the direction of current, potential is positive (+ve).

โœ๏ธ Potential Difference

From A to B (Along Current)

VAB=โˆ’2ร—3=โˆ’6VV_{AB} = -2 \times 3 = -6V


From B to A (Opposite Current)

VBA=+2ร—3=+6VV_{BA} = +2 \times 3 = +6V


2๏ธโƒฃ Battery

๐Ÿ”‹ Given

  • Battery Voltage: 5V

๐Ÿ“Œ Rule

โš ๏ธ Direction of current is not important.

โœ๏ธ Potential Difference

From A to B

VAB=โˆ’5VV_{AB} = -5V


From B to A

VBA=+5VV_{BA} = +5V

๐ŸŽฏ Summary

๐Ÿ”Œ Across a Resistance

โžก๏ธ Along currentV=โˆ’IRV = -IR

โžก๏ธ Opposite to currentV=+IRV = +IR

๐Ÿ”‹ Across a Battery

โžก๏ธ From (+) terminal to (โˆ’) terminalV=โˆ’EV = -E

โžก๏ธ From (โˆ’) terminal to (+) terminalV=+EV = +E

๐Ÿ’ก These sign conventions are used while applying Kirchhoff’s Loop Rule (KVL). ๐Ÿ”„

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