Respuesta :
Answer:
Explanation:
Before the dialectic was inserted the capacitor is Co
When the slab is inserted,
The capacitor becomes
C=kCo
The charge Q is given as
Q=CV
Then, when C=Co
Qo=CoV
Then, when C=kCo
Q=kCoV
Then, the change in charges is given as
Q-Qo= kCoV - CoV
∆Q= kCoV - CoV
Current is given as
I=dQ/dt
I= (kCoV - CoV) / dt
I=Co(kV-V)/dt
Note Co is the value capacitor
So, Capacitance of parallel plates capacitor is given as
Co=εoA/d
Then,
I=εoA(kV-V)/d•dt
I=VεoA(k-1)/d•dt
Where A=πr²
I = V•εo•πr²•(k-1) / d•dt
This is the required expression for current is in the required term
Answer:
[tex]I=V\epsilon_o (K-1) * \frac{r^2}{d*\triangle t}[/tex]
Explanation:
Since a slab is inserted between the plates, so we consider them as two capacitors attached in Parallel. One with dielectric and one without dielectric.
Equation will become:
Total Capacitance=Capacitance With dielectric+ Capacitance without Dielectric
[tex]C=\epsilon_oK*a*\frac{r}{d}+ \epsilon_o(r-a)\frac{r}{d}[/tex]
Where:
a is the distance at which slab is added between the plates.
Rearranging the above equation:
[tex]C=\epsilon_o*\frac{r}{d} [Ka+ (r-a)][/tex]
Charge on the capacitor Q is given by:
Q=CV
Current "I" is given by:
[tex]I=\frac{dQ}{dt}[/tex]
Now,
[tex]I=\frac{d(CV)}{dt} \\\\I=\frac{Vd(C)}{dt} \\I=\frac{Vd[\epsilon_o*\frac{r}{d} [Ka+ (r-a)]]}{dt} \\[/tex]
Taking derivative:
[tex]I=V\epsilon_o}*\frac{r}d}[\frac{d(Ka)}{dt}+\frac{dr}{dt}-\frac{d(a)}{dt}]\\I=V\epsilon_o * \frac{r}{d} (K-1)\frac{d(a)}{dt}[/tex] dr/dt=0 (r is constant)
In the above equation, d(a)/dt is the speed which is constant.
Speed= Distance/time
d(a)/dt= r/Δt
Final Equation will become:
[tex]I=V\epsilon_o * \frac{r}{d} (K-1)\frac{r}{\triangle t} \\I=V\epsilon_o (K-1) * \frac{r^2}{d*\triangle t}[/tex]
