Problem #1
(a) In Fig. 1, what value must R have if the current in the circuit is to be 1.0 mA? Take ε1 = 2.0 V, ε2 = 3.0 V, and r1 = r2 = 3.0 Ω. (b) What is the rate at which thermal energy appears in R?
Fig.1 |
Answer:
Known:
current in the circuit, i = 1.0 mA
emf, ε1 = 2.0 V
emf, ε2 = 3.0 V
internal resistance, r1 = r2 = 1.0 Ω
(a) value must R have if the current in the circuit is to be 1.0 mA is
Assuming the direction of current is counterclockwise and using the loop rule in the counterclockwise direction:
−ε1 − ir2 + ε2 − ir1 − iR = 0
i = (ε2 – ε1)/(r2 + r1 + R)
i = (3.0 V ─ 2.0 V)/(1 Ω + 1 Ω + R)
0.001 = 1/(2 + R)
R = 998 Ω
(b) the rate of thermal energy in R is
P = i2R = (0.001A)2(998 Ω) = 998 μW
Problem #2
A 10-km-long underground cable extends east to west and consists of two parallel wires, each of which has resistance 13 Ω/km. An electrical short develops at distance x from the west end when a conducting path of resistance R connects the wires (Fig. 2). The resistance of the wires and the short is then 100 Ω when measured from the east end and 200 Ω when measured from the west end. What are (a) x and (b) R?
Known:
current in the circuit, i = 1.0 mA
emf, ε1 = 2.0 V
emf, ε2 = 3.0 V
internal resistance, r1 = r2 = 1.0 Ω
(a) value must R have if the current in the circuit is to be 1.0 mA is
Assuming the direction of current is counterclockwise and using the loop rule in the counterclockwise direction:
−ε1 − ir2 + ε2 − ir1 − iR = 0
i = (ε2 – ε1)/(r2 + r1 + R)
i = (3.0 V ─ 2.0 V)/(1 Ω + 1 Ω + R)
0.001 = 1/(2 + R)
R = 998 Ω
(b) the rate of thermal energy in R is
P = i2R = (0.001A)2(998 Ω) = 998 μW
Problem #2
A 10-km-long underground cable extends east to west and consists of two parallel wires, each of which has resistance 13 Ω/km. An electrical short develops at distance x from the west end when a conducting path of resistance R connects the wires (Fig. 2). The resistance of the wires and the short is then 100 Ω when measured from the east end and 200 Ω when measured from the west end. What are (a) x and (b) R?
Answer:
Known:
Resistance, R = 13 Ω/km
cable length, L = 10 km
(a) Let R1 be the resistance on the west side and R2 on the east.
R1 + R2 = 13Ω/km x 10 km = 130 Ω
R2 = 130 – R1
R1 + R + R1 = 2R1 + R = 200 Ω
R2 + R + R2 = 2R2 + R = 100 Ω
Substitute the expression for R2 using R1
2(130 – R1) + R = 100
260 – 100 = 2R1 – R = 160
But, 2R1 + R = 200
Add the two equations
4R1 = 360
R1 = 90 Ω,
R2 = 130 - 90 = 40 Ω, then
x = (90 Ω/130 Ω) x 10 km = 6.9 km
(b) R = 200 – 2(90 Ω) = 20 Ω
Problem #3
A solar cell generates a potential difference of 0.10 V when a 500 Ω resistor is connected across it, and a potential difference of 0.15 V when a 1000 Ω resistor is substituted. What are the (a) internal resistance and (b) emf of the solar cell? (c) The area of the cell is 5.0 cm2, and the rate per unit area at which it receives energy from light is 2.0 mW/cm2. What is the efficiency of the cell for converting light energy to thermal energy in the 1000 Ω external resistor?
Answer:
Known:
area of the cell is A = 5.0 cm2
potential difference when a R1 = 500 Ω resistor is V1 = 0.10 V
potential difference when a R2 = 1000 Ω resistor is V2 = 0.15 V
Known:
Resistance, R = 13 Ω/km
cable length, L = 10 km
(a) Let R1 be the resistance on the west side and R2 on the east.
R1 + R2 = 13Ω/km x 10 km = 130 Ω
R2 = 130 – R1
R1 + R + R1 = 2R1 + R = 200 Ω
R2 + R + R2 = 2R2 + R = 100 Ω
Substitute the expression for R2 using R1
2(130 – R1) + R = 100
260 – 100 = 2R1 – R = 160
But, 2R1 + R = 200
Add the two equations
4R1 = 360
R1 = 90 Ω,
R2 = 130 - 90 = 40 Ω, then
x = (90 Ω/130 Ω) x 10 km = 6.9 km
(b) R = 200 – 2(90 Ω) = 20 Ω
Problem #3
A solar cell generates a potential difference of 0.10 V when a 500 Ω resistor is connected across it, and a potential difference of 0.15 V when a 1000 Ω resistor is substituted. What are the (a) internal resistance and (b) emf of the solar cell? (c) The area of the cell is 5.0 cm2, and the rate per unit area at which it receives energy from light is 2.0 mW/cm2. What is the efficiency of the cell for converting light energy to thermal energy in the 1000 Ω external resistor?
Answer:
Known:
area of the cell is A = 5.0 cm2
potential difference when a R1 = 500 Ω resistor is V1 = 0.10 V
potential difference when a R2 = 1000 Ω resistor is V2 = 0.15 V
For the first circuit:
V1 = ε ─ i1r
V1 = ε ─ (V1/R1)r
0.10 V = ε ─ (0.10 V/500 Ω)r
or 10 = 100ε ─ (10r/500) (*)
For the second circuit:
V2 = ε ─ i2r
V2 = ε ─ (V2/R2)r
0.15 V = ε ─ (0.15 V/1000 Ω)r
or 15 = 100ε ─ (15r/1000) (**)
from (*) and (**),
5 = ─(15r/1000) + (20r/1000)
r = 1000 A
(b) emf of the solar cell is
V1 = ε ─ i1r
0.10 V = ε ─ (0.10 V/500 Ω) x 1000 A
ε = 0.3 V
(c) the efficiency of the cell is
receives energy from light is Prec = 2.0 mW/cm2 = 0.002 W/cm2
eff = P/(Prec.A)
with P = V2/r, then
eff = V2/(Prec.Ar)
eff = (0.15 V)2/(0.002 W/cm2 x 5 cm2 x 1000 Ω) = 0.00225 or 0.25%
Problem #4
In Fig. 4, battery 1 has emf ε1 = 12.0 V and internal resistance r1 = 0.016 Ω and battery 2 has emf ε2 = 12.0 V and internal resistance r2 = 0.012 Ω. The batteries are connected in series with an external resistance R. (a) What R value makes the terminal-to-terminal potential difference of one of the batteries zero? (b) Which battery is that?
Fig.4 |
Answer:
Known:
emfs ε1 = 12.0 V
emfs ε2 = 12.0 V
resistor 1, r1 = 0.016 Ω
resistor 1, r2 = 0.012 Ω
(a) R value makes the terminal-to-terminal potential difference of one of the batteries zero.
The direction of current in this circuit is clockwise, using the loop rule in the clockwise direction:
ε1 − ir2 + ε2 − ir1 − iR = 0 (*)
If the terminal-to-terminal potential difference of one battery is zero, so we have:
εx ─ irX = 0 (**)
and
εy ─ iry = iR
R = (εy/i) ─ ry
X can be 1 or 2, so Y can be 2 or 1 accordingly
So, R = (εy/i) ─ ry = (εy/εx)rx ─ ry
R = rx ─ ry = r1 ─ r2 = 0.016 Ω ─ 0.012 Ω = 4.0 mΩ
(b) battery 1
emfs ε1 = 12.0 V
emfs ε2 = 12.0 V
resistor 1, r1 = 0.016 Ω
resistor 1, r2 = 0.012 Ω
(a) R value makes the terminal-to-terminal potential difference of one of the batteries zero.
The direction of current in this circuit is clockwise, using the loop rule in the clockwise direction:
ε1 − ir2 + ε2 − ir1 − iR = 0 (*)
If the terminal-to-terminal potential difference of one battery is zero, so we have:
εx ─ irX = 0 (**)
and
εy ─ iry = iR
R = (εy/i) ─ ry
X can be 1 or 2, so Y can be 2 or 1 accordingly
So, R = (εy/i) ─ ry = (εy/εx)rx ─ ry
R = rx ─ ry = r1 ─ r2 = 0.016 Ω ─ 0.012 Ω = 4.0 mΩ
(b) battery 1
Post a Comment for "Single Loop Circuits (emf, terminal P.d, internal resistance) Problems and Solutions 2"