GivenAnswer(1-6)
Xc=30 ohm
R1=44 ohm
XL=90 ohm
R2=36 ohm
Impedance (Z) of the circuit is given by
$Z=\sqrt {(R_1+ R_2)^2 + (X_L-X_C)^2}$
$Z=\sqrt {(44+ 36)^2 + (90-30)^2} =100 \Omega $
So Answer for (1) is b
Now current in the circuit is given by
$I=\frac {V}{Z}=200/100=2 A$
So Answer for (2) is c
Impedance of the coil us given by
$Z_c=\sqrt {R_2^2 + X_L^2}$
=97 ohm
So Answer for (3) is a
Now
VC=IXC=2*30=60 V
VR=IR=2*44=88V
VL=IZC=2*97=194 V
VCoil + VRes + VCap= 60 +88+194=342 V
So
A-> Q
B-> P
C-> S
D -> T
Now
Power dissipated is given by
P=I2R
Power dissipated in Coil
P=(2)2*36= 144 W
Power dissipated in Resistor
P= =(2)2*44=176 W
Total power dissipated =144+176=320 W
An Alternating voltage varies with time asAnswer
$V=V_0 sin \omega t$
Given
$V=100 \sqrt {2} sin (100 \pi t)$
Comparing the two equations ,we have
$V_0=100 \sqrt{2} $ Volts
$\omega =100 \pi $ i.e $2 \ pi \nu =100 \pi $
Or frequency=50 Hz
$V_rms= \frac {V_0}{\sqrt 2} =100 Volt$
$V_ms = \ frac {V_0^2}{2} = 10^4 $
The Growth of current in an LR circuit is given byAnswer
I=E/ZAnswer
Where
$Z=\sqrt {R^2 + (X_L - X_C}^2}$
Substituting all the values
Z=11 ohm
So current I =110/11=10 A
Now
VR=IR=10*11=110 V
VL=IXL=10*120=1200 V
VC=IXC=10*120=1200 V
$\sqrt { V_R^2 + (V_L - V_C)^2 }=110 V$
The following quantities are given in the questionAnswer
L=50mH=50X10-3 H
C=20μF=20X10-6F
Vrms=220V
f=50hz or ω=2πf=100π rad/sec
Now
$V_0 = \sqrt {V_rms} = 311$ V
The peak current is given by the below equation in LC circuit
$I_0 = \frac {V_0}{Z}$
Where
$Z = \omega L - \frac { 1}{ \omega C}$
Substituting the values from above
I0=-2.17 A
So magnitude is
I0=2.17 A
$I_{rms}=\frac {I_0}{ \sqrt 2} =1.53$ A
Voltage drop across inductor is given by
VL=IrmsωL=23.1 V
Voltage drop across capacitor is given by
$V_C= \frac {I_{rms}} {\omega C} =243$ V
Since in inductor and capacitor, voltage and current are at right angle, no power will be transferred to them
Hence total power absorbed is also zero
Answer
Answer
$T=2\pi \omega =2 \pi \sqrt {LC}$Answer
Total energy=Initial energy in the inductor
$E=\frac {1}{2} LI^2 =\frac {1}{2} L \frac {V_0^2}{R}$
Answer
Let IL denote the current in the RL branchAnswer
And Ic denote the current in RC Branch
Then Total current through battery
I=IL + IC
Now since the battery is across two branches in parallel the current through the RL branch is unaffected by the presence of the RC branch ,
Now it is given
L=R2C
Or
$\frac {L}{R}=RC$
So
$I=\frac {V_0}{R}$
So I is independent of time and equal to V0/R for t ≥0
Also (1) and (2)
The current will zero in LR branch and have value V0/R in the LC circuit path at t=0
The current will rise with time in the LR circuit and decrease with time in LC circuit
(a) Now from the formula’sAnswer
$T=\frac {1} {f}=\frac {1}{60} sec$
$\omega =2\pi f= 377rad/sec $
$X_L=\omega L=15.08 \Omega $
$Z=\sqrt {R^2 + X_L^2} =25.05 \Omega $
$\phi = tan ^-1 \frac {X_L){R}=37^0 $
Now max current
$I=\frac {V}{Z}=150/25.05=6A$
Max voltage across Resistor is
VR=IR=120V
Max Voltage across Inductor is
VL=IXL =90.5V
(b) At t=T/6
We have
$\omega t=\frac {\pi }{3}=60^0$
Instantaneous current is given by
$i=I sin (\omega t - \phi) =6 sin 23=2.344 A$
Instantaneous voltage across Inductor
$v=V_L cos (\omega t - \phi)=90.5 cos 23=83.29 V$
Instantaneous voltage across Resistor
vR = iR==46.88
Total voltage =vL + vR =130 V
(c)
From the formula’s
$I_rms= \frac {I}{\sqrt 2} =\frac {6}{\sqrt 2} =4.24 A$
$V_rms=\frac {V}{\sqrt 2} = 106.07 V$
Average power= (Irms )2 R=360 W
GivenAnswer
Vrms=240 V ,L=.50H and R=100ohm
Now
Now for time lag,
Voltage of an ac source varies as
$V=V_0 cos \omega t$
And similarly current varies as
$I=I_0 cos (\omega t - \phi )$
Where
$tan \phi =\frac {\omega L}{R}$
Now for t=0,Voltage is maximum
I will be maximum when ωt-Φ=0 i.e when t=Φ/ω
So that time lag between voltage maximum and current maximum is
$\Delta t=\frac{ \phi }{ \omega }$
Now let us calculate Φ
$tan \phi =\frac {\omega L}{R} =\frac {2 \pi (50)(.5)}{100}=1.57$
Or
Φ=57.50=57.5Xπ/180 rad
So time lag
$\Delta t=\frac{ \phi }{ \omega } =3.2 x 10^-3 s$
The effect driving voltage in the circuit will be the power minus the induced EMF in the inductorAnswer
So, Potential difference equation of the circuit will be
$120-.6\frac{dI}{dt}=15I$
Or
$\frac{dI}{dt}=\frac{600-75I}{3} $ ---(1)
At t=0,I is essentially zeroAnswer
So from equation (1)
$\frac{dI}{dt}=\frac{600-75I}{3}$
$\left(\frac{dI}{dt}\right)_{t=0}=\frac{600}{3}=200 $ A/s
Now current reaches it maximum value when current finally stop changing and induced emf becomes zero i.e when \frac{dI}{dt}=0
So maximum current
$0=\frac{600-75I}{3}$
Or
I=8 A
So 80% of current will be =.8*8=.64 A
So from equation (1)
$\frac{dI}{dt}=\frac{600-75I}{3}$
$\frac{dI}{dt}=\frac{600-75*.64}{3}=40$A/s
Now when $\frac{dI}{dt}=150$ A/s
So from equation (1)
$\frac{dI}{dt}=\frac{600-75I}{3}$
I=2 A