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SS3: PHYSICS - 2ND TERM

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  1. Magnetic Field | Week 1
    4 Topics
  2. Electromagnetic Field
    4 Topics
  3. Electromagnetic Induction
    6 Topics
  4. The Transformer
    5 Topics
  5. Simple A.C Circuit
    4 Topics
  6. Models of the Atom
    2 Topics
  7. Radioactivity
    3 Topics
  8. Half Life
    8 Topics
  9. Energy Quantization
    3 Topics
  10. Photoelectric Effect
    4 Topics
  11. Wave Particle Paradox
    3 Topics



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Lesson 5, Topic 2
In Progress

Resistance | Capacitance | Inductance in an A.C Circuit

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Resistance in an A.C Circuit

The a.c current and voltage flowing through a resistor are in phase, they attain a maximum and minimum values at the same time. The value of current is I = I0Sinωt, the voltage, V = V0Sinωt

from Ohm’s law, V = IR, I = \( \frac{V}{R} \)  

Screen Shot 2020 10 29 at 6.48.56 PM

If V = V0Sinωt.

R =\( \frac {V_o Sin \omega t}{I_o Sin \omega t}= \frac{Vrms}{Irms} \) 

R = \( \frac {V_o }{I_o }= \frac{Vrms}{Irms} \)

Irms =  \(\frac{Vrms}{R} \)

Screen Shot 2020 10 29 at 6.49.08 PM

Capacitance in an A.C Circuit

Screen Shot 2020 10 29 at 6.49.20 PM

The voltage (V) and current (I) are out of phase, the current lead the voltage by \( \frac {pi}{2 }\)  or 900 or voltage lags the current by \( \frac {pi}{2 }\)

If capacitor oppose flow of current, hence the opposition offered by a capacitor to flow of an a.c is known as capacitive reactance, Xc

Xc = \( \frac {1}{2 \pi f c} \ \frac{1}{\omega c}\) 

V = IXc

The unit of Xc is ohms.

Xc = capacitive reactance, c = capacitance of capacitor in Farad

f = frequency of the source in Hertz (Hz).


Inductance in A.C Current

Screen Shot 2020 10 29 at 6.49.42 PM

Inductive reactance is the opposition to the flow of an a.c current offered by an inductor.

Screen Shot 2020 10 29 at 6.49.53 PM

VL leads IL by \( \frac {\pi}{2 } \scriptsize \; or \; 90^{\circ}\)

XL= if V = VOsinωt, I = IO \( \left( \scriptsize sin\omega t – \normalsize \frac {\pi}{2 } \right) \)

Since an inductor opposes the flow of current, the inductive reactance is

XL, then V =IXL

XL= 2πfL = ωL

The unit of L is henry (H). The unit XL is (Ω).

A reactance is the opposition to the flow of a.c offered by a capacitor or an inductor or both.

Examples

  1. An inductor of 0.7H is connected to an A.C Source of 220V. Calculate 

(i) Inductive reactance

(ii) current flowing through the circuit

(iii) energy dissipated in the inductor (f =  \( \frac {100}{\pi} \) Hz)

Solution 

(i) XL= 2πfL

= \(\scriptsize 2 \pi \; \times \; \normalsize \frac {100}{\pi} \; \times \; 0.7 \)

= 140Ω

(ii) V = I x L

I = \( \frac {V}{XL} = \frac {220}{140} \)

I = 1.57A

(iii) W = \( \frac {1}{2} \scriptsize LI^2 \)

=  \( \frac {1}{2} \scriptsize \times 0.7 \times 1.57^2 \) 

= 0.86J

2. A 2 F capacitor is connected directly across a 150Vrms, 60Hz a.c source. Find (i) r.m.s value of the current (ii) peak value of the current

Solution 

XC = \( \frac {1}{2 \pi f c}  =\frac {1}{2 \pi \; \times \; 60 \; \times \; 2 \times 10^{-6}f c}  \)  

XC = 1324.4Ω

V = I x C

Irms= \( \frac {V_{rms}}{x_c}  = \frac {150}{1324.4} \)  

Irms = 0.11A

Irms =  \( \frac {I_0}{\sqrt{2}} \)

IO = Irms x √2

= 0.11 x 0.707

=0.160A

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