Let x is the resistance per unit length then equivalent resistance
...(i) also
...(ii) Now
(where y =
) 8y 2 + 8 + 16y = 36y 8y 2 – 20y + 8 = 0 2y 2 – 5y + 2 = 0 2y 2 – 4y – y + 2 = 0 2y (y – 2) – 1(y – 2) = 0 (2y – 1) (y – 2) = 0
or 2
Let x is the resistance per unit length then equivalent resistance
...(i) also
...(ii) Now
(where y =
) 8y 2 + 8 + 16y = 36y 8y 2 – 20y + 8 = 0 2y 2 – 5y + 2 = 0 2y 2 – 4y – y + 2 = 0 2y (y – 2) – 1(y – 2) = 0 (2y – 1) (y – 2) = 0
or 2
Current from D to C = 1A V D – V C = 2 × 1 = 2V V A = 0 V C = 1V, V D – V C = 2 V D – 1 = 2 V D = 3V V D – V B = 2 3 – V B = 2 V B = 1V
For minimum deflection of 1 division required current = 1 µA Voltage required = IR = (1µA) (10) = 10 µV 40 µV ≡ 1ºC 10 µV ≡
ºC = 0.25ºC
Let
be the emf and r be internal resistance of the battery. In the first case,
In the second case,
Divide (i) by (ii), we get
We have,
Current passing through the 9
resistor is
The 9
and 6
resistors are in parallel, therefore
where i is the current delivered by the battery.
Thus, potential difference across 2
resistor is V = iR = 5 × 2 = 10V
(i) When key between the terminals 1 and 2 is plugged in, P.D. across R = IR =
R =
as I = 1A (ii) When key between terminals 1 and 3 is plugged in, P.D. across (X + R) = I(X + R) =
X + R =
X =
R =
and X =
Kirchhoff’s junction law or Kirchhoff’s first law is based on the conservation of charge.
Kirchhoff’s loop law or Kirchhoff’s second law is based on the conservation of energy.
Hence both statements (A) and (B) are correct.
The resistance of length 2R is 12
. Hence the resistance of length R is 6
. Thus two resistances of 6
can be represented as shown in fig. Equivalent resistance R =
Given, Energy = 2 eV = eE E =
V/m
Applying Kirchhoff’s equation to the loop ABFE, – (i 1 + i 2 )R – i 1 r 1 +
= 0
– (i 1 + i 2 )R – i 1 r 1 = 0