Physics MCQs for NEET — Practice Questions with Answers

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The potential differences across the resistance, capacitance and inductance are 80 V, 40 V and 100 V respectively in an L-C-R circuit. The power factor of this circuit is:

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Explanation

The power factor of an L-C-R circuit is given by cosφ, where φ is the phase angle between voltage and current. The given potential differences across R, C, and L are 80V, 40V, and 100V respectively. Using these values, cosφ = 80/√(80^2 + 40^2 + 100^2) = 0.8. Therefore, the power factor is 0.8.

A 100 Ω resistance and a capacitor of 100 Ω reactance are connected in series across a 220 V source. When the capacitor is 50% charged, the peak value of the displacement current is:

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Explanation

impedance of the R-C circuit, Z 
R2+XC2 where, R =100Ω and XC = 100Ω 
 
= 1002Ω 
The peak value of the current, 
Imax=VmaxZ=22021002=2.2 A

An inductor 20 mH, a capacitor 100 μF, and a resistor 50 Ω are connected in series across a source of emf, V= 10sin314t. The power loss in the circuit is:

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A series R-C circuit is connected to an alternating voltage source. Consider two situations:

 
1) When the capacitor is air-filled. 
2) When the capacitor is mica filled. 
Current through the resistor is I and voltage across the capacitor is V then:

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Explanation

In a series R-C circuit, the voltage drop across the capacitor is inversely proportional to the capacitance. When the capacitor is mica-filled, its capacitance increases due to the higher dielectric constant of mica compared to air. Therefore, the voltage drop across the mica-filled capacitor will be lower than the air-filled capacitor for the same current.

In an electrical circuit R, L, C, and an AC voltage source are all connected in series. When L is removed from the circuit, the phase difference between the voltage and the current in the circuit is tan-13. If instead, C is removed from the circuit, the phase difference is again tan-13. The power factor of the circuit is:

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An AC voltage is applied to a resistance R and an inductor L in series. If R and the inductive reactance are both equal to 3Ω, the phase difference between the applied voltage and the current in the circuit is:

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Explanation

In an RL series circuit, the voltage leads the current by a phase angle φ = tan^(-1)(X_L/R). When R = X_L = 3Ω, φ = 45° = π/4 radians. Therefore, the phase difference between applied voltage and current is π/4.

A 220 V input is supplied to a transfer. The output circuit draws a current of 2.0 A at 440 V. If the efficiency of the transformer is 80%, the current drawn by the primary windings of the transformer is:

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Explanation

IS= 2A, ES= 440V, EP=220V 
Efficiency = Output powerinput power=ESISEPIP
80100440×2220×IP

Solving we get- 

IP=5 A

In an AC circuit, the emf (e) and the current (I) at any instant are given respectively by 
e = E0sin wt 
I = I0 sin ωt-ϕ 
The average power in the circuit over one cycle of AC is:

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Explanation

The rate of doing work is known as the power. It is given that in the ac circuit emf is ‘e’ and the current flowing in the circuit is represented by ‘I’ 
e = E0 sin ωt
I=I0sin(ωt-ϕ 
The average power is given by: 
Pavg = W/T 
eIT
E0I0cosϕ×T/2T 
E0I0cosϕ2

What is the value of inductance L for which the current is a maximum in a series LCR circuit with C = 10 μF and ω=1000 s-1?

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Explanation

Given, 
An LCR circuit has a capacitor of capacitance (C) =100 μF , ω=1000 s-1 
In resonance condition, maximum current flows in the circuit. 
Current in LCR series circuit, 
I=VR2+XL-XC2 
Where, V is RMS value of current, R is resistance, XL is inductive reactance and XC is capacitive reactance. 
For current to be maximum, denominator should be minimum which can be done, if 
XL=XC 
We know, 
XL =ωL and XC =1ωC 
This happens in resonance state of the circuit i.e., 
ωL=1ωC 
Or L =1ω2C ……..(i) 
Given, ω=1000 s-1C = 10 μF= 10×10-6 F 
Hence, L =110002×10×10-6 
= 0.1 H 
= 100 mH

The core of a transformer is laminated because :

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Explanation

When magnetic flux linked with a coil changes, induced emf is produced in it and the induced current flows through the wire forming the coil. In 1895, Focault experimentally found that these induced currents are set up in the conductor in the form of closed loops. These currents look like eddies or whirlpools and likewise are known as eddy currents. They are also known as Focault’s current. These currents oppose the cause of their origin, therefore, due to eddy currents, a great amount of energy is wasted in the form of heat energy. If the core of the transformer is laminated, then its effect can be minimized.

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