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Question: In the circuit shown in Figure, the source has a rating of 15 V, 100 Hz. The resistance R is 3 $\Ome...

In the circuit shown in Figure, the source has a rating of 15 V, 100 Hz. The resistance R is 3 Ω\Omega and the reactance of the capacitor is 4 Ω\Omega. It is known that the box certainly contains one or more element (resistance, capacitance or inductance). Which element/s are present inside the box?

A

Only a resistor

B

Only a capacitor

C

Only an inductor

D

An inductor and a capacitor

Answer

Inductor

Explanation

Solution

The circuit shown is a series AC circuit containing a resistor RR, a capacitor CC, and a "Box" whose contents are unknown. We are given the following values:

  • Source voltage (RMS), Vrms=15V_{rms} = 15 V
  • Source frequency, f=100f = 100 Hz
  • Resistance, R=3ΩR = 3 \, \Omega
  • Reactance of the capacitor, XC=4ΩX_C = 4 \, \Omega

The problem asks to identify the element(s) present inside the box. The box is known to contain one or more elements (resistance, capacitance, or inductance).

In series RLC circuits, a common special condition is resonance. At resonance, the inductive reactance (XLX_L) equals the capacitive reactance (XCX_C), making the net reactance of the circuit zero. This results in the total impedance being purely resistive, and the current in the circuit being maximum. Given that the ammeter is shown but no specific reading is provided, it is a common practice in such problems to assume the circuit is operating under a "special" condition, and resonance is the most common such condition for series RLC circuits.

Let's assume the circuit is in resonance.
For a series RLC circuit, the total impedance ZtotalZ_{total} is given by:
Ztotal=(Rtotal)+j(XLtotalXCtotal)Z_{total} = (R_{total}) + j(X_{L_{total}} - X_{C_{total}})
where RtotalR_{total} is the sum of all resistances, XLtotalX_{L_{total}} is the sum of all inductive reactances, and XCtotalX_{C_{total}} is the sum of all capacitive reactances.

In our circuit, we have R=3ΩR = 3 \, \Omega and XC=4ΩX_C = 4 \, \Omega.
Let the elements inside the box contribute resistance RboxR_{box}, inductive reactance XLboxX_{L_{box}}, and capacitive reactance XCboxX_{C_{box}}.

The total resistance in the circuit is Rtotal=R+Rbox=3+RboxR_{total} = R + R_{box} = 3 + R_{box}.
The total inductive reactance in the circuit is XLtotal=XLboxX_{L_{total}} = X_{L_{box}}.
The total capacitive reactance in the circuit is XCtotal=XC+XCbox=4+XCboxX_{C_{total}} = X_C + X_{C_{box}} = 4 + X_{C_{box}}.

For resonance, the net reactance of the circuit must be zero:
XLtotalXCtotal=0X_{L_{total}} - X_{C_{total}} = 0
XLbox(4+XCbox)=0X_{L_{box}} - (4 + X_{C_{box}}) = 0
XLboxXCbox=4ΩX_{L_{box}} - X_{C_{box}} = 4 \, \Omega

This equation tells us that the net reactance of the elements inside the box (Xbox=XLboxXCboxX_{box} = X_{L_{box}} - X_{C_{box}}) must be equal to 4Ω4 \, \Omega.
Since XboxX_{box} is positive, it implies that the inductive reactance inside the box (XLboxX_{L_{box}}) must be greater than the capacitive reactance inside the box (XCboxX_{C_{box}}).

Let's consider the possibilities for the elements inside the box based on this condition:

  1. If the box contains only a resistor (RboxR_{box}): In this case, XLbox=0X_{L_{box}} = 0 and XCbox=0X_{C_{box}} = 0. The condition becomes 00=40 - 0 = 4, which is 0=40 = 4, a contradiction. So, the box cannot contain only a resistor.
  2. If the box contains only a capacitor (CboxC_{box}): In this case, XLbox=0X_{L_{box}} = 0. The condition becomes 0XCbox=40 - X_{C_{box}} = 4, which means XCbox=4ΩX_{C_{box}} = -4 \, \Omega. Reactance values are always positive, so this is impossible. Thus, the box cannot contain only a capacitor.
  3. If the box contains only an inductor (LboxL_{box}): In this case, XCbox=0X_{C_{box}} = 0. The condition becomes XLbox0=4X_{L_{box}} - 0 = 4, so XLbox=4ΩX_{L_{box}} = 4 \, \Omega. This is a valid possibility. If the box contains only an inductor with reactance 4Ω4 \, \Omega, the circuit will be in resonance.
  4. If the box contains a resistor and an inductor (Rbox,LboxR_{box}, L_{box}): The condition XLboxXCbox=4ΩX_{L_{box}} - X_{C_{box}} = 4 \, \Omega still requires XLbox=4ΩX_{L_{box}} = 4 \, \Omega (since XCbox=0X_{C_{box}}=0). This is a valid possibility.
  5. If the box contains a resistor and a capacitor (Rbox,CboxR_{box}, C_{box}): This leads to the same contradiction as case 2.
  6. If the box contains an inductor and a capacitor (Lbox,CboxL_{box}, C_{box}): The condition XLboxXCbox=4ΩX_{L_{box}} - X_{C_{box}} = 4 \, \Omega can be satisfied, e.g., XLbox=5ΩX_{L_{box}} = 5 \, \Omega and XCbox=1ΩX_{C_{box}} = 1 \, \Omega. This is a valid possibility.
  7. If the box contains a resistor, an inductor, and a capacitor (Rbox,Lbox,CboxR_{box}, L_{box}, C_{box}): The condition XLboxXCbox=4ΩX_{L_{box}} - X_{C_{box}} = 4 \, \Omega can be satisfied. This is a valid possibility.

From the analysis, for the circuit to be in resonance, the net reactance of the elements inside the box must be inductive and equal to 4Ω4 \, \Omega. To achieve a net inductive reactance, the box must contain an inductor. It may or may not contain a resistor or a capacitor (as long as XLbox>XCboxX_{L_{box}} > X_{C_{box}} and their difference is 4Ω4 \, \Omega).

Therefore, the only element that is certainly present inside the box, assuming the circuit is at resonance (which is the most common interpretation for such problems when current is not given), is an inductor.