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20 questions
Lenz’s law applies to
Electrostatics
lenses
electromagnetic induction
cinema
slides
Self-induced EMF is sometimes also known as
induced EMF
deduce EMF
back EMF
both a and b
In the relation ϕ=BA cosθ, θ is angle
which normal to surface area makes with direction of magnetic field
which magnetic field makes with the surface
which is never constant
none of these
The cause of induced e.m.f. is
magnetic flux
magnetic field
area
change in magnetic flux
When number of turns of a solenoid is doubled, its self inductance will becomes
2 times
same
8 times
4 times
A capacitor of capacitance C has reactance X. If capacitance and frequency become double, then the capacitive reactance will be
X/4
4X
X/2
2X
The core of a transformer is laminated, so as to
make it robust and strong
reduce energy loss due to eddy current
make it light weight
increase the secondary voltage
If we decrease frequency of source in series R-L-C circuit, impedance may
increase
decrease.
remain same
none of these
Principle of AC generator based on
Fleming right hand rule
Fleming left hand rule
Electro magnetic Induction
Right hand thumb rule
An emf of 200V is induced in a circuit when current in the circuit falls from 5A to 0. A in 0.1 second. The self-inductance of the circuit is-
3.5 H
3.9 H
4 H
4.2 H
The magnetic flux linked with a coil at any instant t is φ=(6t2 -8t+5) Wb, the emf induced in the coil at t= 2 second is-
-16 V
-24 V
16 V
24 V
A metallic cylinder is held vertically and then or small magnet is dropped along its axis. It will fall with-
acceleration a>g
acceleration a˂g
acceleration a=g
acceleration a=0
The magnetic flux through a circuit of resistance R changes by an amount dϕ in time dt , Then the total quantity of electric charge Q , which passing during this time through any point of the circuit is given by
Q = dtdϕ
Q = dtdϕ R
Q = dtdϕ +R
Q = Rdϕ
A conducting square loop of side l and resistance R moves in its plane with a uniform velocity v perpendicular to one of its sides. A magnetic induction B constant in time and space, pointing perpendicular and into the plane at the loop exists everywhere with half the loop outside the field, as shown in figure. The induced e.m.f. is
vBl
vBl/R
RvB
zero
inductive reactance is given by
ωL
ωC1
ωC
ωL1
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