To find the power dissipated in a resistor, we use one of the standard formulas from electric power concepts. The three most common formulas for power \( P \) are:
1. \( P = I^2 R \)
2. \( P = V^2 / R \)
3. \( P = VI \)
Here, we are given:
Current \( I = 2 \, \text{A} \)
Resistance \( R = 10 \, \Omega \)
We are not given the voltage, so the most convenient formula to use is:
\[ P = I^2 R \] Step 1: Square the current
\[ I^2 = (2 \, \text{A})^2 = 4 \, \text{A}^2 \] Step 2: Multiply by resistance
\[ P = 4 \times 10 = 40 \, \text{W} \] Interpretation: The resistor converts 40 joules of electrical energy into heat every second. That’s what we mean by “dissipated power” — energy that’s lost (usually as heat) due to resistance.
Alternative :
We can also find the voltage across the resistor using Ohm’s law:
\[ V = IR = 2 \times 10 = 20 \, \text{V} \]
Now, apply \( P = VI \):
\[ P = 20 \times 2 = 40 \, \text{W} \]
This confirms the same result.
Match List-I with List-II.
Choose the correct answer from the options given below :}
There are three co-centric conducting spherical shells $A$, $B$ and $C$ of radii $a$, $b$ and $c$ respectively $(c>b>a)$ and they are charged with charges $q_1$, $q_2$ and $q_3$ respectively. The potentials of the spheres $A$, $B$ and $C$ respectively are:
Two resistors $2\,\Omega$ and $3\,\Omega$ are connected in the gaps of a bridge as shown in the figure. The null point is obtained with the contact of jockey at some point on wire $XY$. When an unknown resistor is connected in parallel with $3\,\Omega$ resistor, the null point is shifted by $22.5\,\text{cm}$ towards $Y$. The resistance of unknown resistor is ___ $\Omega$. 