---
title: "Electric vectors E, P and D"
subject: "Engineering Physics"
chapter: 7
key: "semester_1/engineering_physics:dielectric-vectors-d-e-p"
source: https://www.bctengineer.com/q/semester_1/engineering_physics/dielectric-vectors-d-e-p
site: BCT Engineering
---

# Electric vectors E, P and D

Engineering Physics · Chapter 7: Electrostatics

- Asked in: 2074 Chaitra, 5 marks; 2072 Kartik, 5 marks; 2068 Shrawan, 5 marks (asked 3 times)
- Video: [Relation between dielectric polarisation, displacement vector and electric field intensity](https://www.youtube.com/watch?v=NaYUFVZ0DKs) — Physics by Kapoor Sir
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_1/engineering_physics/dielectric-vectors-d-e-p
- Whole chapter: https://www.bctengineer.com/md/semester_1/engineering_physics/chapter-7

## Question

Define the three electric vectors E, P and D and develop a relation between them (D = ε0E + P). (Discuss the behaviour of dielectrics in a parallel plate capacitor using Gauss' law.)

## Short answer

E is the total electric field intensity (V/m), P the polarization (dipole moment per unit volume, C/m²), and D = ε₀E + P is the electric displacement (C/m²) whose flux depends only on free charges. In a parallel-plate capacitor with dielectric, Gauss’s law gives σf = ε₀E + P, leading to D = ε₀ε_r E.

## Answer

#### The three vectors
- **Electric field intensity E:** force per unit positive test charge; it is the total field in the dielectric, produced by all (free and bound) charges. Unit: V/m.
- **Polarization P:** electric dipole moment per unit volume of the dielectric. Unit: C/m². For a linear isotropic dielectric P = ε₀ χₑ E, where χₑ is the electric susceptibility.
- **Electric displacement D:** the vector whose flux depends only on free charge; defined as D = ε₀E + P. Unit: C/m².

#### Relation D = ε₀E + P using a parallel-plate capacitor
```text
   + + + + + + + + +   plate, free charge +q (σf = q/A)
   - - - - - - - - -   bound charge -σp (dielectric surface)
   [   dielectric   ]
   + + + + + + + + +   bound charge +σp
   - - - - - - - - -   plate, free charge -q
```
1. Plates carry free surface charge density ±σf. A dielectric slab fills the gap. It becomes polarized, and bound charges of surface density −σp (near the positive plate) and +σp (near the negative plate) appear on its faces.
2. The bound-charge density equals the polarization: σp = P.
3. Apply Gauss' law with a pillbox enclosing the surface of the positive plate and part of the dielectric. The net charge per unit area enclosed is σf − σp:
 ε₀ E = σf − σp = σf − P
4. Rearrange:
 **σf = ε₀E + P**
5. Define D by the Gauss' law for free charge, ∮ D·dA = q_free, so D = σf. Therefore

 **D = ε₀E + P**

#### Dielectric behaviour in the capacitor
- With P = ε₀χₑE: D = ε₀(1 + χₑ)E = ε₀ε_r E = εE, where ε_r = 1 + χₑ is the dielectric constant.
- The field falls to E = E₀/ε_r (E₀ is the field without the dielectric) because the bound charges oppose the free charges.
- At the same charge, the potential difference falls by ε_r, so the capacitance increases to C = ε_r C₀.

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. What is the polarization P?
   A. Force per unit test charge
   B. Total free charge per unit area on a plate
   C. Electric dipole moment per unit volume of the dielectric
   D. Electric dipole moment per unit charge
   Answer: C. P is dipole moment per unit volume (C/m^2); for linear dielectrics P = ε0 χe E. (Key point: Polarization)

2. What is special about the displacement vector D?
   A. It depends only on bound charge
   B. Its flux depends only on the free charge: ∮D·dA = q_free
   C. It equals E in all media
   D. It is the same as P
   Answer: B. D is defined so that Gauss's law for D involves free charge only. (Key point: Meaning of D)

3. In the capacitor derivation, which step leads to D = ε0E + P?
   A. Gauss's law gives ε0E = σf - σp with σp = P, so σf = ε0E + P = D
   B. ε0E = σf + σp, so D = ε0E - P
   C. σp = ε0E, so D = P
   D. The bound charge is ignored in the pillbox
   Answer: A. The enclosed charge per unit area is the free charge minus the bound charge on the slab face, and σp = P. (Key point: Deriving D = ε0E + P)

4. At the same plate charge, what does inserting the dielectric do?
   A. E rises to εr E0 and C falls
   B. E stays the same and C rises
   C. E falls and C falls by εr
   D. E falls to E0/εr and C increases to εr C0
   Answer: D. Bound charges oppose the free charges, lowering E and V while C = q/V rises by εr. (Key point: Effect of the dielectric)

## Related in Engineering Physics

- [Parallel plate capacitor with mica](https://www.bctengineer.com/question.md?key=semester_1%2Fengineering_physics%3Amica-capacitor-field-free-charge) — Engineering Physics, chapter 7
- [Displacement current in parallel plate capacitor](https://www.bctengineer.com/question.md?key=semester_1%2Fengineering_physics%3Adisplacement-current-circular-plates-b-integral) — Engineering Physics, chapter 9
- [Copper slab inserted in capacitor](https://www.bctengineer.com/question.md?key=semester_1%2Fengineering_physics%3Acopper-slab-capacitor-capacitance-change) — Engineering Physics, chapter 7

## Related in other subjects

- [Capacitance of parallel plate capacitor](https://www.bctengineer.com/question.md?key=semester_3%2Felectromagnetism%3Apoisson-parallel-plate-capacitance) — Electromagnetism, chapter 2
- [Parallel plate sheets, field in regions](https://www.bctengineer.com/question.md?key=semester_3%2Felectromagnetism%3Aparallel-plate-sheets-three-regions) — Electromagnetism, chapter 2
- [E due to line charge using Gauss's law](https://www.bctengineer.com/question.md?key=semester_3%2Felectromagnetism%3Aline-charge-field-gauss-law) — Electromagnetism, chapter 2, asked 3×
- [State and explain Gauss's law](https://www.bctengineer.com/question.md?key=semester_3%2Felectromagnetism%3Agauss-law-statement-explain) — Electromagnetism, chapter 2
