When two resistors are connected in parallel, the voltage across each resistor is the same. The power dissipated as thermal energy in a resistor is given by the formula \( P = \frac{V^2}{R} \), where \( V \) is the voltage across the resistor and \( R \) is its resistance.
Let the resistors be \( R_1 = 100 \, \Omega \) and \( R_2 = 200 \, \Omega \).
Since both resistors are in parallel, the voltage \( V \) across both is the same. The power \( P_1 \) for the 100 \(\Omega\) resistor is:
\( P_1 = \frac{V^2}{100} \)
And the power \( P_2 \) for the 200 \(\Omega\) resistor is:
\( P_2 = \frac{V^2}{200} \)
The ratio of thermal energy (power) developed in the 100 \(\Omega\) resistor to that in the 200 \(\Omega\) resistor is:
\(\text{Ratio} = \frac{P_1}{P_2} = \frac{\frac{V^2}{100}}{\frac{V^2}{200}} = \frac{200}{100} = 2:1\)
Thus, the ratio of thermal energy developed in the 100 \(\Omega\) resistor to that in the 200 \(\Omega\) resistor is 2:1.
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is:
Resistance is the measure of opposition applied by any object to the flow of electric current. A resistor is an electronic constituent that is used in the circuit with the purpose of offering that specific amount of resistance.
R=V/I
In this case,
v = Voltage across its ends
I = Current flowing through it
All materials resist current flow to some degree. They fall into one of two broad categories:
Resistance measurements are normally taken to indicate the condition of a component or a circuit.