268520
Three ammeters and with internal resistances ,3r respectively . and parallel and this combination is in series with , The whole combination concted between and . When the battery connected between and , the ratio of the readings of and is
1
2
3
4
Explanation:
Current Electricity
268521
The potential difference between the points and is
1
2
3
4
Explanation:
For the first loop For thesecond loop or or, Therefore, we obtain or, Thus, the p.d across and is
Current Electricity
268522
The resistance of a semicircle shown in fig. betweenitstwo end faces is (G iven that radial thickness , axial thickness , inner radius and resistivity )
1
2
3
4
Explanation:
Here, ohm
Current Electricity
268523
ABCD is a square where each side is a uniform wire of resistance12 . A point lies on such that if a uniform wire of resistance is connected across AE and constant potential difference is applied across and , then and are equipotential .
1
2
3
4
Explanation:
Equivalent resistance between and is For and to be at equal potential, we get Solving Now
268520
Three ammeters and with internal resistances ,3r respectively . and parallel and this combination is in series with , The whole combination concted between and . When the battery connected between and , the ratio of the readings of and is
1
2
3
4
Explanation:
Current Electricity
268521
The potential difference between the points and is
1
2
3
4
Explanation:
For the first loop For thesecond loop or or, Therefore, we obtain or, Thus, the p.d across and is
Current Electricity
268522
The resistance of a semicircle shown in fig. betweenitstwo end faces is (G iven that radial thickness , axial thickness , inner radius and resistivity )
1
2
3
4
Explanation:
Here, ohm
Current Electricity
268523
ABCD is a square where each side is a uniform wire of resistance12 . A point lies on such that if a uniform wire of resistance is connected across AE and constant potential difference is applied across and , then and are equipotential .
1
2
3
4
Explanation:
Equivalent resistance between and is For and to be at equal potential, we get Solving Now
268520
Three ammeters and with internal resistances ,3r respectively . and parallel and this combination is in series with , The whole combination concted between and . When the battery connected between and , the ratio of the readings of and is
1
2
3
4
Explanation:
Current Electricity
268521
The potential difference between the points and is
1
2
3
4
Explanation:
For the first loop For thesecond loop or or, Therefore, we obtain or, Thus, the p.d across and is
Current Electricity
268522
The resistance of a semicircle shown in fig. betweenitstwo end faces is (G iven that radial thickness , axial thickness , inner radius and resistivity )
1
2
3
4
Explanation:
Here, ohm
Current Electricity
268523
ABCD is a square where each side is a uniform wire of resistance12 . A point lies on such that if a uniform wire of resistance is connected across AE and constant potential difference is applied across and , then and are equipotential .
1
2
3
4
Explanation:
Equivalent resistance between and is For and to be at equal potential, we get Solving Now
268520
Three ammeters and with internal resistances ,3r respectively . and parallel and this combination is in series with , The whole combination concted between and . When the battery connected between and , the ratio of the readings of and is
1
2
3
4
Explanation:
Current Electricity
268521
The potential difference between the points and is
1
2
3
4
Explanation:
For the first loop For thesecond loop or or, Therefore, we obtain or, Thus, the p.d across and is
Current Electricity
268522
The resistance of a semicircle shown in fig. betweenitstwo end faces is (G iven that radial thickness , axial thickness , inner radius and resistivity )
1
2
3
4
Explanation:
Here, ohm
Current Electricity
268523
ABCD is a square where each side is a uniform wire of resistance12 . A point lies on such that if a uniform wire of resistance is connected across AE and constant potential difference is applied across and , then and are equipotential .
1
2
3
4
Explanation:
Equivalent resistance between and is For and to be at equal potential, we get Solving Now