The galvanometer resistance is 30 Ω and it is connected to 2 V battery along with a resistance 2000 Ω in series. A full scale deflection of 25 divisions is obtained. In order to reduce this deflection to 20 divisions, the resistance in series should be
2470 Ω
2370 Ω
2180 Ω
2210 Ω
A.
2470 Ω
Total initial resistance = RG + R
= 30 + 2000
= 2030Ω
And connected with battery E = 2V
Current i = A
as the full-scale deflection scale for
1 mA = 25 divisions
Let x be the effective resistance of the circuit, then
2V = 2030 × × 103
= x ×
⇒ x =
⇒ x = 2500 Ω
∴ Resistance to be added= 2500 - 30 = 2470 Ω
A thin bar magnet of length 2 L is bent at the mid-point so that the angle between them is 60°. The new length of the magnet is
L/2√3
√3 L/2
L
2 L/3
The magnetic flux through each turn of a coil having 200 turns is given as (t2 1) x 10-3 Wb, where t is in second. The emf induced in the coil at t = 3s is
0.7 V
1.2 V
0.8 V
0.9 V
A vessel of depth t is half filled with a liquid having refractive index n1 and the other half is filled with water of having refractive index n2. The apparent depth of the vessel as viewed from top is
In photoelectric effect, the number of photo-electrons emitted is proportional to
velocity of incident beam
frequency of incident beam
intensity of incident beam
work function for cathode material
A change of 8.0 mA in the emitter current brings a change of 7. 9 mA in the collector current. The value of a will be
0.96
0.93
0.90
0.99
The half-life of 198Au is 2.7 days. The average life is
4 days
3.4 days
3.9 days
None of the above
The de-Broglie wavelength of electron falling on the target in an X-ray tube is),. The cut-off wavelength of the emitted X-ray is
If MO is the mass of an oxygen isotope 8O17 Mp and Mn are the masses of a proton and a neutron, respectively, the nuclear binding energy of the isotope is
MO c2
( MO - 17Mn ) c2
(MO - 8Mp ) c2
( 8 Mp + 9 Mn - MO)
A nucleus disintegrates into two nuclear parts which have their velocities in the ratio 2 : 1. The ratio of their nuclear size will be
21/3 : 1
1 : 31/2
31/2 : 1
1 : 21/2