LR, RC and LCR Circuits - NEET Physics Chapterwise MCQs & PYQs

NEET LR, RC and LCR Circuits MCQs & PYQs

Question 41:

easy

Assertion (A): If the resistance of a series resonant LCR circuit is decreased, then the peak current versus frequency graph will be taller and narrower.


Reason (R): If the resistance of a series resonant LCR circuit decreased, then its resonance will be unaffected.


 

When resistance \(R\) in a series \(LCR\) circuit decreases, the peak current \(I_{max} = V/R\) at resonance increases, making the peak taller. The quality factor \(Q = (\omega_0 L)/R\) increases, leading to a narrower resonance curve. The resonant frequency \(omega_0 = 1/\sqrt{LC}\) remains unchanged, but the overall resonance behavior (sharpness, peak current) is affected. Therefore, (A) is true and (R) is false.

Question 42:

easy

Assertion (A): The impedance of series L-C-R circuit can be greater, equal or less than the resistance.


Reason (R): The minimum impedance of series LCR circuit depends over angular frequency of applied emf.


 

The impedance of a series \(LCR\) circuit is given by \(Z = \sqrt{R^2 + (X_L - X_C)^2}\). Since \((X_L - X_C)^2\) is always non-negative, \(Z\) is always greater than or equal to \(R\). Thus, (A) is false. The minimum impedance occurs at resonance, where \(Z_{min} = R\). This minimum value depends only on \(R\) and not on the angular frequency \(omega\). Thus, (R) is also false.

Question 43:

easy

Assertion (A): When frequency is greater than resonance frequency in a series LCR circuit, it will be an inductive circuit.


Reason (R): Resultant Voltage Will lead the current.


 

When frequency \(f > f_r\) in a series LCR circuit, the inductive reactance \(X_L\) is greater than the capacitive reactance \(X_C\). This makes the circuit inductive. In an inductive circuit, the resultant voltage leads the current. Hence, both assertion and reason are true, and the reason correctly explains the assertion.

Question 44:

easy

Assertion (A): In ac supply we cannot feel any fluctuations of current in bulbs.


Reason (R): House hold ac supply has very low frequency.


 

Our eyes cannot detect flickers above \(10-15 \text{ Hz}\). Household AC supply (\(50/60 \text{ Hz}\)) changes too rapidly for us to perceive fluctuations in bulbs. Thus, Assertion (A) is true. However, \(50/60 \text{ Hz}\) is not considered a "very low frequency", thus Reason (R) is false.

Question 45:

Assertion (A): An electric lamp is connected in series with a long solenoid of copper with air core and then connected to \( \text{ac} \) source. If an iron rod is inserted in solenoid, the lamp will become dim.


Reason (R): If an iron rod is inserted in solenoid, the inductance of solenoid increases.


 

Inserting an iron rod (ferromagnetic material) into a solenoid significantly increases its inductance \( L \) (R is true). In an \( \text{ac} \) circuit, this increases inductive reactance \( X_L =\omega L \), which in turn increases the total impedance \( Z \) of the circuit. Higher \( Z \) leads to lower current \( I = V/Z \), making the lamp dim (A is true). (R) provides the correct explanation for (A).

Question 46:

easy

Assertion (A): For an electric lamp connected in series with a variable capacitor and \( \text{ac} \) source, its brightness increases with increase of capacitance.


Reason (R): Capacitive reactance decreases with increase in capacitance of capacitor.


 

Capacitive reactance is given by \( X_C = frac{1}{omega C} \). As capacitance \( C \) increases, \( X_C \) decreases (R is true). A decrease in \( X_C \) leads to a decrease in the total circuit impedance \( Z \). With constant voltage \( V \), a lower \( Z \) results in higher current \( I = V/Z \), thus increasing the lamp's brightness (A is true). (R) correctly explains (A).

Question 47:

easy

Assertion (A): In series RL circuit voltage leads the current.


Reason (R): In series \( \text{LCR} \) circuit current may lead the voltage.

In a series \( text{RL} \) circuit, the inductive reactance \( X_L \) causes the voltage to lead the current, so (A) is true. In a series \( text{LCR} \) circuit, if \( X_C > X_L \), the circuit is capacitive, and current leads the voltage, so (R) is true. Both statements are true, but (R) is about a different circuit type and does not explain (A).

Question 48:

easy

Consider the following statements and choose the correct option.


Statement A: Capacitive reactance is inversely proportional to frequency.


Statement B: Inductive reactance is directly proportional to frequency.


 

The formulae are \(X_C = \frac{1}{2\pi f C}\) (inversely proportional) and \(X_L = 2\pi f L\) (directly proportional). Hence, both statements are correct.

Question 49:

moderate

An a.c. voltage given by relation, \(V = 300\sin(100t)\text{ volt}\) is connected with resistor having resistance \(60\ \Omega\) and inductor of inductance \(L\). If peak current in the circuit is \(3\text{ A}\), the value of \(L\) will be (where \(t\) denotes the time in s)

Short Solution: 

Peak voltage \(V_0 = 300\text{ V}\), peak current \(I_0 = 3\text{ A}\), so impedance \(Z = V_0/I_0 = 100\ \Omega\). Using \(Z = \sqrt{R^2 + (\omega L)^2}\), we have \(100 = \sqrt{60^2 + (100L)^2}\), which gives \(100L = 80 \implies L = 0.8\text{ H}\).

Detailed Solution: 

Understanding the Given Problem

We are given a standard alternating current (AC) circuit containing a resistor and an unknown inductor connected in series.
Given Data:
  • AC Voltage Equation: $V = 300\sin(100t)\text{ V}$
  • Resistance ($R$): $60\ \Omega$
  • Peak Current ($I_0$): $3\text{ A}$
From the standard AC voltage equation $V = V_0\sin(\omega t)$, we can extract two crucial values by comparing it to our given equation:
  • Peak Voltage ($V_0$): $300\text{ V}$
  • Angular Frequency ($\omega$): $100\text{ rad/s}$

Step 1: Calculate the Total Impedance ($Z$)

In an AC circuit, the total opposition to the current flow is called impedance ($Z$). It can be found using the peak voltage and peak current, similar to Ohm's law:
$$Z = \frac{V_0}{I_0}$$
Substitute the known values:
$$Z = \frac{300\text{ V}}{3\text{ A}} = 100\ \Omega$$

Step 2: Use the L-R Circuit Impedance Formula

For a series L-R circuit, the impedance is the vector sum of the resistance ($R$) and the inductive reactance ($X_L$). The formula is:
$$Z = \sqrt{R^2 + X_L^2}$$
We also know that inductive reactance is given by $X_L = \omega L$. Substituting this into the impedance formula gives:
$$Z = \sqrt{R^2 + (\omega L)^2}$$

Step 3: Solve for the Inductance ($L$)

Now, substitute the values we have gathered ($Z = 100\ \Omega$, $R = 60\ \Omega$, $\omega = 100\text{ rad/s}$) into the equation:
$$100 = \sqrt{60^2 + (100L)^2}$$
Square both sides of the equation to remove the square root:
$$(100)^2 = 60^2 + (100L)^2$$
$$10000 = 3600 + (100L)^2$$
Subtract $3600$ from both sides:
$$6400 = (100L)^2$$
Take the square root of both sides:
$$80 = 100L$$
Finally, solve for $L$:
$$L = \frac{80}{100} = 0.8\text{ H}$$

Final Answer

The correct value of the inductance $L$ is 0.8 H, which corresponds to Option 3.

Question 50:

easy

Consider a series \(LCR\) circuit in which reactance and resistance are \(100\ \Omega\) each. When the circuit is connected to ac source \(220\text{ V}\), \(50\text{ Hz}\), then current drawn from the source is

Here, \(R = 100\ \Omega\) and net reactance \(X = 100\ \Omega\). Total impedance is \(Z = \sqrt{R^2 + X^2} = 100\sqrt{2}\ \Omega\). The current \(I = \frac{V}{Z} = \frac{220}{100\sqrt{2}} = 1.1\sqrt{2}\text{ A}\).