To solve the problem, let's analyze the behavior of an LCR circuit at resonance.
Concept Explanation: At resonance, an LCR circuit has its inductive reactance equal to its capacitive reactance, and the circuit impedance is purely resistive. The impedance \(Z\) is given by the resistance \(R\) alone, thus:
\(Z = R\)
The current amplitude \(I_0\) at resonance is given by:
\(I_0 = \frac{V}{R}\)
where \(V\) is the peak voltage applied across the circuit.
Problem Statement Analysis:
Initially, for a resistance \(R\), the current at resonance is:
\(I_0 = \frac{V}{R}\)
Now, the resistance is halved to \(R/2\), while the inductance \(L\) and capacitance \(C\) remain the same. Hence, the new current amplitude \(I'_0\) is:
\(I'_0 = \frac{V}{R/2} = \frac{2V}{R} = 2I_0\)
Conclusion: The current amplitude at resonance will be double the initial current amplitude when the resistance is halved, assuming all other parameters remain constant.
Therefore, the correct answer is double.
At resonance, impedance is given by:
\[ Z = R. \]
The current in the circuit is:
\[ I = \frac{V}{R}. \]
When the resistance \(R\) is halved:
\[ R \to \frac{R}{2}, \quad I \to 2I. \]
Thus, the current amplitude becomes double.
Final Answer: Double.
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 : \(A_2 \rightleftharpoons 2A\)