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 \( 26 \, \Omega \).
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :
A full wave rectifier circuit with diodes (\(D_1\)) and (\(D_2\)) is shown in the figure. If input supply voltage \(V_{in} = 220 \sin(100 \pi t)\) volt, then at \(t = 15\) msec:
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.