\(${14 \,\Omega}$\) and \(${40 \,\Omega}$\)
\(${40 \,\Omega}$\) and \(${14 \,\Omega}$\)
\(${40 \,\Omega}$\) and \(${30 \,\Omega}$\)
\(${14 \,\Omega}$\) and \(${30 \,\Omega}$\)
Potential difference across \(${ 20 \,\Omega} = 20 \times 1$\) \($= {20 \, V}$\) = potential difference across \($R_2$\) Current in \($R_2 = 0.5 \, A$\) \($\therefore \:\: R_{2 } = \frac{20 V}{0.5 A} = 40 \Omega$\) Potential difference across \($R_1 = {69 \, V - 20 \, V} $\) \($={49 \, V}$\) Current in \($R_1 = 0.5 {A + \frac{20}{10} A + \, A = 3.5 \, A}$\) \($\therefore \:\:\: R_1 = \frac{49}{3.5} = 14 \, \Omega$\)
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.