In the figure shown below, a resistance of 150.4 $ \Omega $ is connected in series to an ammeter A of resistance 240 $ \Omega $. A shunt resistance of 10 $ \Omega $ is connected in parallel with the ammeter. The reading of the ammeter is ______ mA.
This problem involves a circuit with a voltage source, a series resistor, and an ammeter shunted by another resistor. We need to find the reading of the ammeter, which is the current flowing through it.
The solution requires the application of several fundamental circuit laws:
Step 1: Calculate the equivalent resistance of the parallel combination of the ammeter and the shunt resistor.
The ammeter has a resistance \( R_A = 240 \, \Omega \), and the shunt resistor has a resistance \( R_{sh} = 10 \, \Omega \). These two are connected in parallel. \[ R_p = \frac{R_A \times R_{sh}}{R_A + R_{sh}} \] \[ R_p = \frac{240 \times 10}{240 + 10} = \frac{2400}{250} = 9.6 \, \Omega \]
Step 2: Calculate the total equivalent resistance of the entire circuit.
The series resistor \( R_s = 150.4 \, \Omega \) is connected in series with the parallel combination \( R_p \). \[ R_{eq} = R_s + R_p \] \[ R_{eq} = 150.4 + 9.6 = 160 \, \Omega \]
Step 3: Calculate the total current flowing from the voltage source.
The voltage of the source is \( V = 20 \, \text{V} \). Using Ohm's Law: \[ I_{total} = \frac{V}{R_{eq}} = \frac{20}{160} = \frac{1}{8} \, \text{A} \] \[ I_{total} = 0.125 \, \text{A} \]
Step 4: Calculate the current flowing through the ammeter using the current divider rule.
The total current \( I_{total} \) splits between the ammeter (\( R_A \)) and the shunt resistor (\( R_{sh} \)). The reading of the ammeter is the current flowing through it, \( I_A \). \[ I_A = I_{total} \times \frac{R_{sh}}{R_A + R_{sh}} \] \[ I_A = 0.125 \times \frac{10}{240 + 10} \] \[ I_A = 0.125 \times \frac{10}{250} = 0.125 \times \frac{1}{25} \] \[ I_A = \frac{0.125}{25} = 0.005 \, \text{A} \]
Step 5: Convert the ammeter reading to milliamperes (mA).
To convert from amperes to milliamperes, we multiply by 1000. \[ I_A = 0.005 \, \text{A} \times 1000 \, \frac{\text{mA}}{\text{A}} = 5 \, \text{mA} \]
The reading of the ammeter is 5 mA.
$R_{eq} = R_1 + R_2$
$R_{eq} = 150.4 + \frac{240 \times 10}{250}$
$R_{eq} = 150.4 + 9.6 = 160 \Omega$
$I_1 = \frac{IR_2}{240}$
$I_1 = \frac{I \times 9.6}{240}$
$I = \frac{20}{160}$
$I_1 = \frac{20}{160} \times \frac{9.6}{240} = \frac{1}{200} = 5 \times 10^{-3} A = 5 mA$
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,




What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)