A dielectric slab of thickness $$d$$ is inserted in a parallel plate capacitor whose negative plate is at $$x = 3d$$. The slab is equidistant from the plates. The capacitor is given some charge. As $$x$$ goes from $$0$$ to $$3d$$ :
Explanation
Three charges $$Q$$, $$+q$$ and $$+q$$ are placed at the vertices of a right angled isosceles triangle as shown in the figure. The net electrostatic energy of the configuration is zero if $$Q$$ is equal to :
An alpha particle of $$5 MeV$$ at a large distance proceeds towards a gold nucleus $$(Z=79)$$ to make a head on collision. The closest distance of approach from the centre of gold nucleus is:
Using
$$ Energy=\dfrac{1}{2} \times C_{equivalent}\times V^2 $$
We need to find the equivalent capacitance of the capacitor.
Using law for series combination of capacitors,
$$ \dfrac{1}{C_{net}} = \dfrac{1}{C_1} + \dfrac{1}{C_2} + \dfrac{1}{C_3} $$
where, $$ C_1 = \dfrac{A\epsilon_0}{x} $$ ( x is the width between capacitor walls and dielectric on one side )
$$C_2 = \dfrac {A\epsilon_0\kappa}{(\dfrac{d}{2})} = \dfrac{4A\epsilon_0}{d} $$
$$C_3 = \dfrac{A\epsilon_0}{(\dfrac{d}{2}-x)}$$
therefore,
$$\dfrac{1}{C_{net}} = \dfrac{x}{(A\epsilon_0)} + \dfrac{(\dfrac{d}{2}-x)}{(A\epsilon_0)} + \dfrac{d}{(4A\epsilon_0)} = \dfrac{3d}{(4A\epsilon_0)} \Rightarrow C_{net} = \dfrac{4A\epsilon_0}{3d} $$
Therefore energy $$= \dfrac{2A\epsilon_0 V^2}{3d} $$
The capacitance of a parallel plate capacitor is given by
$$C = \dfrac {\varepsilon_o \varepsilon_r A}{d}$$,
where $$A$$ is the area of the plate and $$d$$ is the distance between them.
In the first case, there was no dielectric medium, i.e., $$\varepsilon_r = 1$$.
So we have $$C = \dfrac {\varepsilon_o A}{d}$$
In the second case, the distance is doubled, i.e., $$2d$$ and a substance of dielectric constant $$3$$ is inserted between the plates.
Hence capacitance will change to
$$C' = \dfrac {3 \varepsilon_o A}{2d}$$
So, $$ \dfrac{C'}{C} = \dfrac {3}{2}$$
$$ \implies C' = \dfrac {3}{2} C$$
For option (B) solution : In XWY, charge on capacitor plate =KCE
In XYW, charge on capacitor plate = CE
For option (C) solution : In WXY, U = $$\displaystyle \frac {1} {2} KCE^2 $$
In XYW, U = $$\displaystyle \frac {CE^2} {2K} $$
For option (D) solution : 2 both cases, electric field = $$\displaystyle \frac {E} {d} $$ .
Potential for each plate remain same over whole are if potential difference thems is way V then V = Ed i.e. E is also same inside the plates
To Keep E same free change dansity is changed i.e. charge redistributes itself
To find new capacitance, two capacitors can be taken as connected in parallel Then
$$\displaystyle C_{eq}=\frac{5.\epsilon _{0}A/3}{d}+\frac{\epsilon _{0}.2A/3}{d}=\frac{7\epsilon _{0}A}{3d}$$
Q = CV, as Q remains unchanged V is changed to $$\displaystyle \frac{3}{7}V$$
Please disable the adBlock and continue. Thank you.