alternatively_current_ physics concept, Summaries of Physics

Solutions to exercises related to AC circuits. The exercises cover topics such as resistance, inductance, capacitance, impedance, and resonance. The solutions provide step-by-step calculations for determining values such as rms current, net power consumed, Q-value, angular frequency, and energy stored. One exercise involves a radio tuning over a frequency range and requires the calculation of the capacitance of a variable capacitor. useful for students studying electrical engineering or physics.

Typology: Summaries

2021/2022

Available from 04/06/2023

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Exercises
Question 7.1:
A 100 โ„ฆ resistor is connected to a 220 V, 50 Hz ac supply.
(a) What is the rms value of current in the circuit?
(b) What is the net power consumed over a full cycle?
Answer 7.1:
Resistance of the resistor, R = 100 โ„ฆ
Supply voltage, V = 220 V
Frequency, ฮฝ = 50 Hz
(a) The rms value of current in the circuit is given as
๐ผ=๐‘‰
๐‘…=220
100=2.20 ๐ด
(b) The net power consumed over a full cycle is given as:
P = VI = 220 ร— 2.2 = 484 W
Question 7.2:
(a) The peak voltage of an ac supply is 300 V. What is the rms voltage?
(b) The rms value of current in an ac circuit is 10 A. What is the peak
current?
Answer 7.2:
(a) Peak voltage of the ac supply, V0 = 300 V
rms voltage is given as:
๐‘‰= ๐‘‰๐‘œ
โˆš2=300
โˆš2=212.1 ๐‘‰
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Exercises

Question 7.1:

A 100 ฮฉ resistor is connected to a 220 V, 50 Hz ac supply.

(a) What is the rms value of current in the circuit? (b) What is the net power consumed over a full cycle? Answer 7.1:

Resistance of the resistor, R = 100 ฮฉ

Supply voltage, V = 220 V

Frequency, ฮฝ = 50 Hz

(a) The rms value of current in the circuit is given as ๐ผ =

(b) The net power consumed over a full cycle is given as:

P = VI = 220 ร— 2.2 = 484 W

Question 7.2:

(a) The peak voltage of an ac supply is 300 V. What is the rms voltage? (b) The rms value of current in an ac circuit is 10 A. What is the peak current? Answer 7.2: (a) Peak voltage of the ac supply, V 0 = 300 V rms voltage is given as:

๐‘‰ =

(b) The rms value of current is given as: I = 10 A Now, peak current is given as: ๐ผ๐‘œ = โˆš2๐ผ = โˆš2 ร— 10 = 14.1 ๐ด

Question 7.3:

A 44 mH inductor is connected to 220 V, 50 Hz ac supply. Determine the

rms value of the current in the circuit.

Answer 7.3:

Inductance of inductor, L = 44 mH = 44 ร— 10โˆ’^3 H

Supply voltage, V = 220 V

Frequency, ฮฝ = 50 Hz Angular frequency, ฯ‰ = 2๐œ‹ฮฝ Inductive reactance, XL = ฯ‰ L = 2๐œ‹ฮฝL = 2๐œ‹ ร— 50 ร— 44 ร— 10โˆ’3^ ฮฉ

rms value of current is given as:

๐‘‹๐ฟ^ =^

2๐œ‹ ร— 50 ร— 44 ร— 10โˆ’3^ = 15.92 ๐ด

Hence, the rms value of current in the circuit is 15.92 A.

Question 7.4:

A 60 ฮผF capacitor is connected to a 110 V, 60 Hz ac supply. Determine the

rms value of the current in the circuit.

Answer 7.4:

Capacitance of capacitor, C = 60 ฮผF = 60 ร— 10โˆ’^6 F

For a pure inductive circuit, the phase difference between alternating voltage

and current is 90ยฐ i.e., ๐›ท= 90ยฐ.

Hence, P = 0 i.e., the net power is zero.

In the capacitive circuit,

rms value of current, I = 2.49 A

rms value of voltage, V = 110 V

Hence, the net power absorbed can be obtained as:

๐‘ƒ = ๐‘‰๐ผ ๐ถ๐‘œ๐‘  ๐›ท

For a pure capacitive circuit, the phase difference between alternating

voltage and current is 90ยฐ i.e., ๐›ท = 90ยฐ.

Hence, P = 0 i.e., the net power is zero.

Question 7.6:

Obtain the resonant frequency ฯ‰r of a series LCR circuit with L = 2.0 H,

C = 32 ฮผF and R = 10 ฮฉ. What is the Q-value of this circuit?

Answer 7.6:

Inductance, L = 2.0 H

Capacitance, C = 32 ฮผF = 32 ร— 10โˆ’^6 F

Resistance, R = 10 ฮฉ

Resonant frequency is given by the relation,

โˆš2 ร— 32 ร— 10โˆ’^

8 ร— 10โˆ’3^ = 125 ๐‘Ÿ๐‘Ž๐‘‘/๐‘ .

Now, Q-value of the circuit is given as:

32 ร— 10โˆ’^

10 ร— 4 ร— 10โˆ’^

Hence, the Q-Value of this circuit is 25.

Question 7.7:

A charged 30 ฮผF capacitor is connected to a 27 mH inductor. What is the

angular frequency of free oscillations of the circuit?

Answer 7.7:

Capacitance, C = 30ฮผF = 30ร—10โˆ’^6 F Inductance, L = 27 mH = 27 ร— 10โˆ’^3 H

Angular frequency is given as:

๐œ”๐‘Ÿ =

โˆš27 ร— 10โˆ’3^ ร— 30 ร— 10โˆ’^

9 ร— 10โˆ’4^ = 1.11 ร— 10

Hence, the angular frequency of free oscillations of the circuit is 1.11 ร— 10^3 rad/s.

Question 7.8:

Suppose the initial charge on the capacitor in Exercise 7.7 is 6 mC. What is

the total energy stored in the circuit initially? What is the total energy at later

time?

Answer 7.8:

Capacitance of the capacitor, C = 30 ฮผF = 30ร—10โˆ’^6 F

Current in the circuit can be calculated as:

๐ผ =

Hence, the average power transferred to the circuit in one complete cycle:

VI = 200 ร— 10 = 2000 W.

Question 7.10:

A radio can tune over the frequency range of a portion of MW broadcast

band: (800 kHz to 1200 kHz). If its LC circuit has an effective inductance of

200 ฮผH, what must be the range of its variable capacitor?

[Hint: For tuning, the natural frequency i.e., the frequency of free oscillations

of the LC circuit should be equal to the frequency of the radio wave.]

Answer 7.10:

The range of frequency (ฮฝ) of a radio is 800 kHz to 1200 kHz.

Lower tuning frequency, ฮฝ 1 = 800 kHz = 800 ร— 10^3 Hz

Upper tuning frequency, ฮฝ 2 = 1200 kHz = 1200 ร— 10^3 Hz

Effective inductance of circuit L = 200 ฮผH = 200 ร— 10โˆ’^6 H

Capacitance of variable capacitor for ฮฝ 1 is given as:

๐ถ 1 =

Where,

ฯ‰ 1 = Angular frequency for capacitor C 1 = 2๐œ‹๐œˆ 1 = 2๐œ‹ ร— 800 ร— 10^3 ๐‘Ÿ๐‘Ž๐‘‘/๐‘ 

(2๐œ‹ ร— 800 ร— 10^3 )^2 ร— 200 ร— 10โˆ’

= 1.9809 ร— 10โˆ’10^ ๐น = 198 ๐‘๐น

Capacitance of variable capacitor for ฮฝ 2 is given as:

๐ถ 2 =

Where,

ฯ‰ 2 = Angular frequency for capacitor C 2 = 2๐œ‹๐œˆ 2 = 2๐œ‹ ร— 1200 ร— 10^3 ๐‘Ÿ๐‘Ž๐‘‘/๐‘ 

(2๐œ‹ ร— 1200 ร— 10^3 )^2 ร— 200 ร— 10โˆ’

= 0.8804 ร— 10โˆ’10^ ๐น = 88 ๐‘๐น

Hence, the range of the variable capacitor is from 88.04 pF to 198.1 pF.

Question 7.11:

Figure 7.21 shows a series LCR circuit connected to a variable frequency 230 V source. L = 5.0 H, C = 80ฮผF, R = 40 ฮฉ

Where,

๐‘‰๐‘œ = Peak voltage = โˆš2 ๐‘‰

โˆด ๐ผ๐‘œ =

โˆš2 ร— 230

Hence, at resonance, the impedance of the circuit is 40 ฮฉ and the amplitude

of the current is 8.13 A.

(c) rms potential drop across the inductor, (VL)rms = I ร— ฯ‰rL

Where,

๐ผrms =

โˆด (๐‘‰๐ฟ)rms =

ร— 50 ร— 5 = 1437.5 ๐‘‰

Potential drop across the capacitor:

โˆด (๐‘‰๐ถ )rms = ๐ผ ร—

4 ร—^

50 ร— 80 ร— 10โˆ’6^ = 1437.5 ๐‘‰

Potential drop across the resistor:

(๐‘‰๐‘… )rms = ๐ผ๐‘… =

4 ร— 40 = 230 ๐‘‰

Potential drop across the LC combination: ๐‘‰๐ฟ๐ถ = ๐ผ(๐‘‹๐ฟ โˆ’ ๐‘‹๐ถ ) At resonance, ๐‘‹๐ฟ = ๐‘‹๐ถ โ‡’ ๐‘‰๐ฟ๐ถ = 0 Hence, it is proved that the potential drop across the LC combination is zero

at resonating frequency.