CHAPTER 4
ELECTROSTATICS II
Student Book
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7. Where do we find capacitors in real life?
8. What is the symbol of capacitors?
9. To move a point charge through a potential difference of 10 ³V requires 2x1
of work. What is the magnitude of the charge?
10. Calculate the potential difference between two points which are 20crn a
30cm from an isolated point charge of 3 x 10-8c in a vacuum.
harge of 5C from A to B, if the pot

Verified Answer :

Certainly! Let's address each question step-by-step.

7. Where do we find capacitors in real life?

Capacitors are found in a wide range of real-life applications, including:
- Electronic devices like smartphones, laptops, and televisions
- Power supply circuits to smooth out voltage fluctuations
- Radio frequency circuits, such as those in tuning radios
- Electric motors and air conditioners to improve efficiency and power factor correction
- Camera flashes to quickly release stored energy
- Energy storage in applications like uninterruptible power supplies (UPS)

8. What is the symbol of capacitors?

The symbol for a capacitor consists of two parallel lines, one representing each plate of the capacitor. It looks like this:
``
| |

``
In the context of schematic diagrams, it can also be represented with a "+" and "-" sign if it is a polarized capacitor, such as an electrolytic capacitor.

9. To move a point charge through a potential difference of \(\( 10^3 \, \text{V} \)\) requires \(\( 2 \times 10^{-3} \, \text{J} \)\) of work. What is the magnitude of the charge?

To determine the magnitude of the charge, \(\( q \)\), we can use the relationship between work (W), charge (q), and potential difference (V):

\(\[ W = q \cdot V \]\)

Rearranging to solve for \(\( q \)\):

\(\[ q = \frac{W}{V} \]\)

Given:
\(\[ W = 2 \times 10^{-3} \, \text{J} \]\)
\(\[ V = 10^3 \, \text{V} \]\)

Substituting the values:

\(\[ q = \frac{2 \times 10^{-3}}{10^3} = 2 \times 10^{-6} \, \text{C} \]\)

Therefore, the magnitude of the charge is \(\( 2 \times 10^{-6} \, \text{C} \)\).

10. Calculate the potential difference between two points which are 20 cm and 30 cm from an isolated point charge of \(\( 3 \times 10^{-8} \, \text{C} \)\) in a vacuum.

To determine the potential difference between two points at distances \(\( r_1 \)\) and \(\( r_2 \)\) from a point charge \(\( q \)\), we use the formula for the electric potential \(\( V \)\) at a distance \(\( r \)\) from a point charge:

\(\[ V = \frac{k \cdot q}{r} \]\)

Where:
- \(\( k \)\) is Coulomb's constant, approximately \(\( 9 \times 10^9 \, \text{N} \cdot \text{m}^2/\text{C}^2 \)\)

The potential difference \(\( \Delta V \)\) between the two points is:

\(\[ \Delta V = V_1 - V_2 = \frac{kq}{r_1} - \frac{kq}{r_2} \]\)

Given:
\(\[ q = 3 \times 10^{-8} \, \text{C} \]\)
\(\[ r_1 = 20 \, \text{cm} = 0.2 \, \text{m} \]\)
\(\[ r_2 = 30 \, \text{cm} = 0.3 \, \text{m} \]\)

Substituting these values:

\(\[ \Delta V = \frac{9 \times 10^9 \times 3 \times 10^{-8}}{0.2} - \frac{9 \times 10^9 \times 3 \times 10^{-8}}{0.3} \]\)

\(\[ \Delta V = \frac{27 \times 10^1}{0.2} - \frac{27 \times 10^1}{0.3} \]\)

\(\[ \Delta V = 1350 \, \text{V} - 900 \, \text{V} \]\)

\(\[ \Delta V = 450 \, \text{V} \]\)

Therefore, the potential difference between the two points is \(\( 450 \, \text{V} \)\).