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![[Post New]](/templates/default/images/icon_minipost_new.gif) 21 May 2008 15:32:19 IST
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An ammeter isconverted to voltmeter by connecting a
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 21 May 2008 20:35:29 IST
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To use an ammeter as a voltmeter, connect it in series with a known high resistance, this causes a current to flow that is relative to the voltage applied (ohms law).
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The Scientist does not study nature because it is useful; he studies it because he delights in it, & he delights in it because it is beautiful. If nature were not beautiful, it would not be worth knowing, life would not be worth living. Ofcourse I do not here speak of that beauty that strikes the senses, the beauty of qualities & appearances; not that I undervalue such beauty, far from it, but it has nothing to do with science; I mean that profounder beauty which comes from the harmoniuos order of the parts, & which a pure intelligence can grasp. |
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 21 May 2008 20:38:10 IST
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AMMETER | | Ammeter is an electrical measuring device, which is used to measure electric current through the circuit. It is the modified form of galvanometer | CONNECTION OF AMMETER IN CIRCUIT | | An ammeter is always connected in series to a circuit. | |
SYMBOL | | | | CONVERSION OF GALVANOMETER
INTO AMMETER | | Since Galvanometer is a very sensitive instrument therefore it can’t measure heavy currents. In order to convert a Galvanometer into an Ammeter, a very low resistance known as "shunt" resistance is connected in parallel to Galvanometer. Value of shunt is so adjusted that most of the current passes through the shunt. In this way a Galvanometer is converted into Ammeter and can measure heavy currents without fully deflected. | VALUE OF SHUNT RESISTANCE | | Let resistance of galvanometer = Rg and it gives full-scale deflection when current Ig is passed through it. Then, | Vg = IgRg -------(i) | Let a shunt of resistance (Rs) is connected in parallel to galvanometer. If total current through the circuit is I. | | Then current through shunt: | Is = (I-Ig) | potential difference across the shunt: | Vs= IsRs | or
Vs = (I – Ig)Rs -------(ii) | But | Vs =Vg
(I - Ig)Rs = IgRg
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VOLT METER | | Voltmeter is an electrical measuring device, which is used to measure potential difference between two points in a circuit. | |
CONNECTION OF VOLTMETER IN CIRCUIT | | Voltmeter is always connected in parallel to a circuit. | SYMBOL | | | CONVERSION OF GALVANOMETER INTO VOLTMETER | | Since Galvanometer is a very sensitive instrument, therefore it can not measure high potential difference. In order to convert a Galvanometer into voltmeter, a very high resistance known as "series resistance" is connected in series with the galvanometer. | VALUE OF SERIES RESISTANCE | | Let resistance of galvanometer = Rg and resistance Rx (high) is connected in series to it. Then combined resistance = (Rg + Rx). | | If potential between the points to be measured = V and if galvanometer gives full-scale deflection, when current "Ig" passes through it. Then, | | V = Ig (Rg + Rx)
V = IgRg + IgRx
V – IgRg = IgRx
Rx = (V – IgRg)/Ig
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Thus Rx can be found. |
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The Scientist does not study nature because it is useful; he studies it because he delights in it, & he delights in it because it is beautiful. If nature were not beautiful, it would not be worth knowing, life would not be worth living. Ofcourse I do not here speak of that beauty that strikes the senses, the beauty of qualities & appearances; not that I undervalue such beauty, far from it, but it has nothing to do with science; I mean that profounder beauty which comes from the harmoniuos order of the parts, & which a pure intelligence can grasp. |
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![[Post New]](/templates/default/images/icon_minipost_new.gif) 21 May 2008 20:41:02 IST
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edison is perfectly right
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Ken
From: UNITED STATES, Green Bay, Wisconsin
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