A galvanometer has 30 divisions and a sensitivity 16 It can be converted into a voltmeter to read 3 V by connecting (approximately):
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In a circuit, 5 percent of total current passes through a galvanometer. If the resistance of the galvanometer is G then the value of the shunt is :
⇒
⇒
A voltmeter has a range 0-V with a series resistance R. With a series resistance 2R, the range is 0-V'. The correct relation between V and V' is :
For conversion of galvanometer (of resistances) into voltmeter, a resistance R is connected in series.
∴ and
⇒ ⇒
⇒ ⇒
If an ammeter is to be used in place of a voltmeter then we must connect with the ammeter a :
If ammeter is used in place of voltmeter (i.e. in parallel) it may damage due to large current in circuit. Hence to control this large amount of current a high resistance must be connected in series.
A galvanometer of resistance 36 Ω is changed into an ammeter by using a shunt of 4 Ω. The fraction f0 of total current passing through the galvanometer is :
A galvanometer, having a resistance of 50 Ω gives a full scale deflection for a current of 0.05 A. The length in meter of a resistance wire of area of cross-section 2.97× 10–2 cm2 that can be used to convert the galvanometer into an ammeter which can read a maximum of 5 A current is (Specific resistance of the wire = 5 × 10–7 Ωm)
⇒ ⇒ .
An ammeter reads up to 1 ampere. Its internal resistance is 0.81 ohm. To increase the range to 10 A the value of the required shunt is :
⇒ .
The dimension of the magnetic field intensity B is:
(b) F = Bil
An electron moves with a constant speed v along a circle of radius r. Its magnetic moment will be (e is the electron's charge)
(b)
The field normal to the plane of a wire of n turns and radius r which carries a current i is measured on the axis of the coil at a small distance h from the centre of the coil. This is smaller than the field at the centre by the fraction
(a) Field at the centre
Field at a distance h from the centre
(By binomial theorem)
Hence is less than by a fraction
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