A parallel plate capacitor is formed by two large, flat, conducting plates, which – [Free] B50

A parallel plate capacitor is formed by two large, flat, conducting plates, which are parallel to each other. The left plate has a surface charge density of + 𝜎 +Οƒ The right plate has a surface charge density of βˆ’ 𝜎 βˆ’Οƒ Find the electric field vectors (magnitude and direction) at the following regions:

A parallel plate capacitor is formed by two large, flat, conducting plates, which - [Free] B50
Electric Field Between Two Charged Plates – Detailed Explanation

🧲 Electric Field Due to Two Parallel Plates

Two infinite parallel plates are given:

  • The left plate has a surface charge density of +Οƒ.
  • The right plate has a surface charge density of βˆ’Οƒ.

πŸ“˜ Basic Formula: Electric Field from a Charged Plate

The electric field due to a single infinite sheet of charge is given by:

E = Οƒ / (2Ξ΅β‚€)

Direction:

  • Positive charge (+Οƒ) β†’ field points away from the plate.
  • Negative charge (βˆ’Οƒ) β†’ field points toward the plate.

πŸ“ Region-wise Electric Field Calculation

a) Left of the Plates

Field from left plate: leftward β†’ \( \frac{Οƒ}{2Ξ΅β‚€} \)
Field from right plate: rightward β†’ \( \frac{Οƒ}{2Ξ΅β‚€} \)

Fields cancel out: Eleft = 0 N/C

b) Between the Plates

Field from left plate: rightward β†’ \( \frac{Οƒ}{2Ξ΅β‚€} \)
Field from right plate: rightward β†’ \( \frac{Οƒ}{2Ξ΅β‚€} \)

Fields add up: Ebetween = Οƒ / Ξ΅β‚€

c) Right of the Plates

Field from left plate: rightward β†’ \( \frac{Οƒ}{2Ξ΅β‚€} \)
Field from right plate: leftward β†’ \( \frac{Οƒ}{2Ξ΅β‚€} \)

Fields cancel out: Eright = 0 N/C

πŸ“Š Final Summary Table

Region Electric Field Magnitude Direction
Left of the Plates 0 N/C β€”
Between the Plates Οƒ / Ξ΅β‚€ To the right
Right of the Plates 0 N/C β€”

Similar Posts

Leave a Reply

Your email address will not be published. Required fields are marked *