Alternating Current

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New answer posted

a month ago

0 Follower 3 Views

A
alok kumar singh

Contributor-Level 10

Power delivered = 1000 W
Voltage = 220 V
Transmission 'I' = 1000/220
Power loss = I²R
Efficiency = (1000x100)/ (1000 + I²R)

New answer posted

a month ago

0 Follower 8 Views

A
alok kumar singh

Contributor-Level 10

Kindly go through the solution

 

New answer posted

2 months ago

0 Follower 3 Views

A
alok kumar singh

Contributor-Level 10

C = ε 0 A d X C = 1 C ω = d ε 0 A ω l 0 = V 0 X C = V 0 ε 0 A ω d = 2 π f V 0 ε 0 A d

l 0 = 2 * 3 . 1 4 * 5 0 * 2 0 * 8 . 8 5 * 1 0 1 2 * 1 2 * 1 0 3 = 2 7 . 7 9 * 1 0 6 A = 2 7 . 7 9 μ A              

New answer posted

2 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

Power is maximum at resonance

So, X L = X C = 1 ω C

C = 1 ω * X L

= 1 2 5 0 * 1 0 0 * π 2

= 4 μ F [ π 2 = 1 0 ]

New answer posted

2 months ago

0 Follower 4 Views

V
Vikash Kumar Vishwakarma

Contributor-Level 7

The inductor generates induced electromotive force (EMF) and opposes the changes in the current flow. Due to this the current lag the voltage by 90 degrees.

New answer posted

2 months ago

0 Follower 5 Views

P
Payal Gupta

Contributor-Level 10

v = 100 sin ωt

i0=100Rx=5Rx=20Ω

i = 5sin(ωtπ2)

i = 100 5sin ωt

5=100RyRy=1005=20Ω

When x and y both are connected in series :-

v = 100sin ωt

tan = 1 = 45°

R0Rx2+Ry2=202Ω

l0o=v0R0=100202=52A.

lms=l02

=522

=52A=52A

New answer posted

2 months ago

0 Follower 5 Views

V
Vishal Baghel

Contributor-Level 10

At very high frequencies

XC=1ωC0

XL=ωL

Thus equivalent circuit

Z=1+2+2=5Ω

l=2205=44A

New answer posted

2 months ago

0 Follower 2 Views

V
Vishal Baghel

Contributor-Level 10

 P1=cos? =Rz=RXL2+R2

P1=cos? =RR2=12

So,  P1P2=12

New answer posted

2 months ago

0 Follower 2 Views

P
Payal Gupta

Contributor-Level 10

Z=R2+ (XLXC)2

Z= (120)2+ (10100)2=150Ω

ω=1LC=1101*104=105

? ω=2πf

f=1032π10=50Hz

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