A parallel plate capacitor of capacitance C is charged to a potential V and then disconnected with the battery. If separation between the plates is decreased by `50%` and the space between the plates is filled with a dielectric slab of dielectric constant `K=10`. then
A parallel plate capacitor of capacitance C is charged to a potential V and then disconnected with the battery. If separation between the plates is decreased by `50%` and the space between the plates is filled with a dielectric slab of dielectric constant `K=10`. then
A
P.d. between the plates increases by `95%`
B
P.d. between the plates decreases by `50%`
C
P.d. between the plates increases by `50%`
D
P.d. between the plates decreases by `95%`
Text Solution
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The correct Answer is:
To solve the problem step by step, we will analyze the situation of a parallel plate capacitor when the separation between the plates is decreased and a dielectric slab is introduced.
### Step 1: Understand the initial conditions
The initial capacitance \( C \) of the capacitor is given by the formula:
\[
C = \frac{K \epsilon_0 A}{D}
\]
where:
- \( K \) is the dielectric constant (initially \( K = 1 \) since there is no dielectric),
- \( \epsilon_0 \) is the permittivity of free space,
- \( A \) is the area of the plates,
- \( D \) is the separation between the plates.
### Step 2: Determine the charge on the capacitor
When the capacitor is charged to a potential \( V \), the charge \( Q \) on the capacitor can be expressed as:
\[
Q = C \cdot V
\]
Since the capacitor is disconnected from the battery, the charge \( Q \) remains constant.
### Step 3: Analyze the new conditions after decreasing the plate separation
When the separation between the plates is decreased by 50%, the new separation \( D' \) is:
\[
D' = \frac{D}{2}
\]
### Step 4: Introduce the dielectric slab
Now, we fill the space between the plates with a dielectric slab of dielectric constant \( K = 10 \). The new capacitance \( C' \) can be calculated as:
\[
C' = \frac{K \epsilon_0 A}{D'}
\]
Substituting \( D' \):
\[
C' = \frac{10 \epsilon_0 A}{\frac{D}{2}} = \frac{20 \epsilon_0 A}{D}
\]
### Step 5: Relate the new capacitance to the initial capacitance
Since the initial capacitance \( C \) was:
\[
C = \frac{\epsilon_0 A}{D}
\]
We can express the new capacitance \( C' \) in terms of \( C \):
\[
C' = 20 C
\]
### Step 6: Calculate the new potential difference
Since the charge \( Q \) remains constant, we can relate the new potential difference \( V' \) to the new capacitance:
\[
Q = C' \cdot V' \implies V' = \frac{Q}{C'}
\]
Substituting \( Q = C \cdot V \) and \( C' = 20C \):
\[
V' = \frac{C \cdot V}{20C} = \frac{V}{20}
\]
### Step 7: Calculate the percentage decrease in potential
The percentage decrease in potential can be calculated as:
\[
\text{Percentage Decrease} = \frac{V - V'}{V} \times 100
\]
Substituting \( V' = \frac{V}{20} \):
\[
\text{Percentage Decrease} = \frac{V - \frac{V}{20}}{V} \times 100 = \frac{20V - V}{20V} \times 100 = \frac{19V}{20V} \times 100 = 95\%
\]
### Conclusion
Thus, the potential difference between the plates decreases by 95%.
To solve the problem step by step, we will analyze the situation of a parallel plate capacitor when the separation between the plates is decreased and a dielectric slab is introduced.
### Step 1: Understand the initial conditions
The initial capacitance \( C \) of the capacitor is given by the formula:
\[
C = \frac{K \epsilon_0 A}{D}
\]
where:
...
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