We are given the following formula for power:
\(P = \frac{V^2}{R}\)
Using the formula for power, we can calculate the resistance \( R_b \) as:
\(R_b = \frac{V^2}{P} = \frac{10000}{500} = 20 \, \Omega\)
Next, we use Ohm's law to find the current. From Ohm's law, we know:
\(i = \frac{V}{R_b} = \frac{130}{R}\)
We now set up the equation by equating the current expressions:
\(\frac{100}{20} = \frac{130}{R}\)
Solving for \( R \), we get:
\(R = \frac{130 \times 20}{100} = 26 \, \Omega\)
The resistance \( R \) is \( 26 \, \Omega \).
In a Vernier caliper, \(N+1\) divisions of vernier scale coincide with \(N\) divisions of main scale. If 1 MSD represents 0.1 mm, the vernier constant (in cm) is:
Current electricity is defined as the flow of electrons from one section of the circuit to another.
There are two types of current electricity as follows:
The current electricity whose direction remains the same is known as direct current. Direct current is defined by the constant flow of electrons from a region of high electron density to a region of low electron density. DC is used in many household appliances and applications that involve a battery.
The current electricity that is bidirectional and keeps changing the direction of the charge flow is known as alternating current. The bi-directionality is caused by a sinusoidally varying current and voltage that reverses directions, creating a periodic back-and-forth motion for the current. The electrical outlets at our homes and industries are supplied with alternating current.