1.

A dielectric of relative permittivity (dielectric constant ) k completely fills the space betweenthe plates of a parallel-plate capacitor with a surface charge density sigma. Show that (i) the induced density of surface charge on the dielectric is sigma_(p)=sigma(1-(1)/(k)) (ii) the capacitance of the capacitor is increased by a factor equal to the ratio of the electric field without the dielectric to that with the dielectric.

Answer»

Solution :CONSIDER a parallel-plate capacitor without a dielectric, of plate area A, plate separation d and capacitance `C_(0),` charged to a potential difference V and then isolated.
Suppose the free charges on its conducting plates are +Q and -Q, FIG. (a). The surface density of free charge is
`sigma =(Q)/(A) ""` ...(1)
If A is very large and d is very small, the electric field in the region between the plates is almost uniform, except at the edges. The magnitude of the electric field intensity is
`E_(0)=(V)/(d)=(sigma)/(epsilon_(0))=(Q)/(epsilon_(0)A) "" ` (2)
Now, suppose a dielectric completely fills the space the charged plates. A polarisation charge - `Q_(p)` appears on the exterior surface of the dielectric nearer to the POSITIVE platewhile a polarisation charge `+Q_(p)` appears on its opposite face. Since the capacitor was isolated after charging, the free charge Q on the plates is the same as earlier.

Consider the Gaussian surface S as shown in Fig. (b). It encloses free charge +Q on the left plate and the bound polarisation charge - `Q_(p)` on the surface of the dielectric.
The net charge enclosed by `S=Q-Q_(p).`
`therefore` By Gauss's theorem, the TNEI over the Gaussian surface is
`epsilon_(0) underset(s) int vecE* d vecS=epsilon_(0)EA=Q-Q_(p)`
`therefore` The magnitude of the electric field intensity in the dielectric is
`E=(Q-Q_(p))/(epsilon_(0)A)=(Q)/(epsilon_(0)A)-(Q_(p))/(epsilon_(0)A)=(sigma)/(epsilon_(0))-(sigma_(p))/(epsilon_(0)) "" ` ...(3)
Writing `E=(E_(0))/(k),` where k is the relative permittivity (dielectric CONSTANT) of the MEDIUM, `(E_(0))/(k)=(sigma)/(epsilon_(0))-(sigma_(p))/(epsilon_(0))`
` therefore (sigma)/(k epsilon_(0))=(sigma)/(epsilon_(0))-(sigma_(p))/(epsilon_(0))`
`therefore (sigma)/(k)=sigma-sigma_(p)`
`therefore` The surface density of induced charge is
`sigma_(p)=sigma-(sigma)/(k)=sigma(1-(1)/(k)) "" ` ...(4)
Without the dielectric, the capacitance of the capacitor is, `C_(0)=Q//V.`
`therefore Q=C_(0)V=C_(0)E_(0)d "" ` ...(5)
Let the capacitancewith the dielectric be C. Since the free charge Q remains the same,`Q=CEd "" `...(6)
Equating the right hand sides of Eqs. (5) and (6),
`CEd = C_(0)E_(0)d`
`therefore C=C_(0)((E_(0))/(E))=kC_(0) "" ` ...(7)
Thus, the capacitance increases by the factor of `k=E_(0)//E.`


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