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Growth of current circuit
• 𝑉
𝑠 − 𝑅 𝑖 − 𝐿
𝑑𝑖
𝑑𝑡
= 0
• Rearranging
•
di(t)
dt
+
Ri(t)
L
=
𝑉𝑠
L
; it is of the form
𝑑𝑦
𝑑𝑥
+ p x ∗ y = q(x)
• Integrating factor 𝑒 𝑃 𝑥 𝑑𝑥
= 𝑒
𝑅
𝐿
𝑑𝑡
= 𝑒
𝑅
𝐿
𝑡
. Multiplying this on both sides
• 𝑒
𝑅
𝐿
𝑡 𝑑𝑖(𝑡)
𝑑𝑡
+ 𝑒
𝑅
𝐿
𝑡 Ri(t)
𝐿
= 𝑒
𝑅
𝐿
𝑡 𝑉𝑠
𝐿
•
𝑑 (𝑒
𝑅
𝐿𝑡
∗i t )
𝑑𝑡
= 𝑒
𝑅
𝐿
𝑡 𝑉𝑠
𝐿
//Rewriting
•
𝑑 (𝑒
𝑅
𝐿𝑡
∗i t )
𝑑𝑡
𝑑𝑡 = 𝑒
𝑅
𝐿
𝑡 𝑉𝑠
𝐿
𝑑𝑡 //Integrating on both sides
• 𝑒
𝑅
𝐿
𝑡
∗ i t =
𝑉𝑠
𝐿
𝑒
𝑅
𝐿
𝑡
∗
𝐿
𝑅
+ 𝐾 => i t =
𝑉𝑠
𝑅
+ 𝐾𝑒−
𝑅
𝐿
𝑡
• Applying initial condition at t=t0; i(t)=I0
• 𝐾 = 𝐼0 −
𝑉𝑠
𝑅
𝑒
𝑅
𝐿
𝑡0
• Substituting in i(t)
• i t =
𝑉𝑠
𝑅
−
𝑉𝑠
𝑅
−𝐼0 𝑒−
𝑅
𝐿
(𝑡−𝑡0)
If t=0; I0 =0
𝐢 𝐭 =
𝑽𝒔
𝑹
𝟏 − 𝒆−
𝑹𝒕
𝑳
𝒗𝑳 𝐭 = 𝐋
𝒅𝒊
𝒅𝒕
= 𝑽𝒔𝒆−
𝑹𝒕
𝑳
Charging of a capacitor
• 𝑉
𝑠 − 𝑅C
𝑑 𝑉𝑐 𝑡
𝑑𝑡
− Vc(t) = 0
• Rearranging
•
d𝑉𝑐(𝑡)
dt
+
𝑉𝑐 t
RC
=
𝑉𝑠
RC
; it is of the form
𝑑𝑦
𝑑𝑥
+ p x ∗ y = q(x)
• Integrating factor 𝑒 𝑃 𝑥 𝑑𝑥
= 𝑒
1
𝑅𝐶
𝑑𝑡
= 𝑒
1
𝑅𝐶
𝑡
. Multiplying this on both
sides
• 𝑒
1
𝑅𝐶
𝑡 d𝑉𝑐 t
dt
+ 𝑒
1
𝑅𝐶
𝑡 𝑉𝑐 t
RC
= 𝑒
1
𝑅𝐶
𝑡 𝑉𝑠
RC
•
𝑑 (𝑒
1
𝑅𝐶𝑡
∗𝑉𝑐 t )
𝑑𝑡
= 𝑒
1
𝑅𝐶
𝑡 𝑉𝑠
RC
• Integrating on both sides
•
𝑑 (𝑒
1
𝑅𝐶𝑡
∗𝑽𝒄 𝐭 )
𝑑𝑡
= 𝑒
1
𝑅𝐶
𝑡 𝑉𝑠
RC
• 𝑒
1
𝑅𝐶
𝑡
∗ 𝑽𝒄 𝐭 = 𝑒
1
𝑅𝐶
𝑡
𝑉
𝑠 + 𝐾
• 𝑽𝒄 𝐭 = 𝑉
𝑠 + 𝐾𝑒−
1
𝑅𝐶
𝑡
• Applying initial condition at t=t0; Vc(t)=V0
• 𝐾 = (𝑉0 − 𝑉𝑆)𝑒
1
𝑅𝐶
𝑡0
• Substituting in 𝑽𝒄 𝐭
• 𝑽𝒄 𝐭 = 𝑽𝒔 − (𝑽𝑺 − 𝑽𝟎)𝒆−
𝟏
𝑹𝑪
(𝒕−𝒕𝟎)
If t=0; V0 =0
𝑽𝒄 𝐭 = 𝑽𝒔(𝟏 − 𝒆−
𝒕
𝑹𝑪)
𝒊 𝐭 = 𝑪
𝒅𝑽𝒄 𝐭
𝒅𝒕
=
𝑽𝒔
𝑹
𝒆−
𝒕
𝑹𝑪
• If a given circuit is not in the form of standard RL/RC circuit. It can be
converted to its thevenin’s equivalent across the inductor/capacitor.
Eg Numerical 6)
• For the circuit shown in figure below, the switch S has been closed for
a long time and then opens at t = 0.
Find,
i. vab(0−
)
ii. ix 0−
iii. iL 0−
iv. ix(0+
)
v. vab(0+
)
vi. ix(t = ∞)
vii. vab(t = ∞)
viii.ix t , for t > 0
Solution:
There is a current (I0) flowing in the inductor before switch is opened. To determine
I0, Analyze the circuit before the switch is operated.
𝐢 𝐭 =
𝑽𝒔
𝑹
𝟏 − 𝒆−
𝑹𝒕
𝑳
𝑽𝒔=Vth=12.857
R=Rth=2.142Ω
𝐢 𝐭 =
𝟏𝟐. 𝟖𝟓𝟕𝟏
𝟐. 𝟏𝟒𝟐
𝟏 − 𝒆−
𝟐.𝟏𝟒𝟐𝒕
𝟏 = 𝟔 𝟏 − 𝒆−
𝟐.𝟏𝟒𝟐𝒕
𝟏
1
0

6

5

1
H
2
0
V
a
b
i
x
5

2
0
V
a
b
1
0

i
x Since the switch is closed for a long time.
Inductor behaves as a short circuit carrying a
current 6A.
i. vab 0− ⇒ 0. Behaves as a short circuit
ii. ix 0− ⇒ 6 ∗
10
15
= 4𝐴
iii. iL 0− ⇒ 6𝐴
10
6
5
1H
20V
a
b
ix
𝐢 𝐭 =
𝑽𝒔
𝑹
−
𝑽𝒔
𝑹
−𝑰𝟎 𝒆−
𝑹
𝑳
(𝒕−𝒕𝟎)
t0 = 0
I0=6A
Vs=Vth=20V
R=Rth=5Ω
𝐢 𝐭 =
𝟐𝟎
𝟓
−
𝟐𝟎
𝟓
− 𝟔 𝒆−
𝟓
𝟏
(𝒕−𝟎)
𝐢 𝐭 = 𝟒 − 𝟒 − 𝟔 𝒆−𝟓𝒕
𝐢 𝐭 = 𝟒 + 𝟐𝒆−𝟓𝒕
iv. ix 0
+
⇒ 𝑖𝐿 0
+
= 6𝐴
v. vab(0+
) ⇒ 20 − 5𝑖𝐿 0
+
− 𝑉𝑎𝑏 = 0 ⇒ Vab = −10V
vi. ix(t = ∞) ⇒ 𝑖𝐿 ∞ = 4𝐴
vii. vab t = ∞ = 0V. Inductor behaves as a short
Before the switch is opened the current would reach a maximum of 6A .
Therefore I0=6A
For t>0
Numerical 7)
For the circuit shown in figure below, the switch S has been kept open
for a long time and then it is closed at t = 0.
Find,
i. vc(0−
)
ii. vc 0+
iii. ic 0−
iv. ic(0+
)
v.
dvc
dt t=0+
vi. vc t = ∞
vii. find the time constants of the circuit before and after the switch is
closed
1
0

4
0
V
4
F
before the switch is operated
𝐕𝐜 𝐭 = 𝑽𝒔 𝟏 − 𝒆−
𝟏
𝑹𝑪
𝒕
Vc t = 40 1 − 𝑒−
1
40
𝑡
Capacitor is charged to a maximum of 40 V
before the switch is operated. Hence behaves as
an open circuit.
vc 0−
= 40V; ic 0−
= 0A
𝝉1 = 40s
After the switch is operated
𝐕𝐜 𝐭 = 𝑽𝒔 − (𝑽𝑺 − 𝑽𝟎)𝒆−
𝟏
𝑹𝑪
(𝒕−𝒕𝟎)
Vs=Vth=15V
R=Rth= 3.75Ω
Vc t = 15 − 15 − 40 𝑒−
1
15
𝑡−0
Vc t = 15 + 25 𝑒−
1
15𝑡
vc 0+ = 40V; vc ∞ = 15V; 𝝉2 = 15s
1
0

4
0
V
4
F
6

𝑑Vc 0+
𝑑𝑡
= −
5
3
𝐶
𝑑Vc 0+
𝑑𝑡
= −
20
3
Numerical 8)
For the circuit shown below, switch S is kept in position ‘1’ for a long
time and then it is moved to position ‘2’ at time 𝑡 = 0 . Find
i. The current expression for 𝐢 𝐭 for 𝑡 ≥ 0
ii. Calculate the time constants of the circuit before and after the
switching phases
10
25V
5
10 2
10
5A
5
10 2
Solution
Switch in position 1
𝐕𝐜 𝐭 = 𝑽𝒔 𝟏 − 𝒆−
𝟏
𝑹𝑪
𝒕
Vs=Vth=10V
R=Rth=6Ω
𝝉1= R*C=12µ
𝑽𝒄 𝒕 = 𝟏𝟎 𝟏 − 𝒆
−
𝟏
𝟏𝟐µ𝒕
10
30V
10 2
Switch in position 2
𝐕𝐜 𝐭 = 𝑽𝒔 − (𝑽𝑺 − 𝑽𝟎)𝒆−
𝟏
𝑹𝑪
(𝒕−𝒕𝟎)
Vs=Vth=15V
R=Rth= 5Ω
𝝉2= R*C=10µ
Vc t = 15 − 15 − 10 𝑒
−
1
10µ
𝑡−0
𝑽𝒄 𝒕 = 𝟏𝟓 − 𝟓𝒆
−
𝟏
𝟏𝟎µ
𝒕
𝑖𝑐 = 𝐶
d𝑉𝑐(𝑡)
dt
= 2µ ∗ −5𝑒
−
1
10µ
𝑡
∗ −
1
10µ
= 𝑒
−
1
10µ
𝑡
𝑖10 =
Vc t
10
= 1.5 − 0.5𝑒
−
1
10µ
𝑡
𝒊𝑿 = 𝟏. 𝟓 + 𝟎. 𝟓𝒆
−
𝟏
𝟏𝟎µ 𝒕

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RL RC _src - Basic electric theory .pptx

  • 1.
  • 2. Growth of current circuit • 𝑉 𝑠 − 𝑅 𝑖 − 𝐿 𝑑𝑖 𝑑𝑡 = 0 • Rearranging • di(t) dt + Ri(t) L = 𝑉𝑠 L ; it is of the form 𝑑𝑦 𝑑𝑥 + p x ∗ y = q(x) • Integrating factor 𝑒 𝑃 𝑥 𝑑𝑥 = 𝑒 𝑅 𝐿 𝑑𝑡 = 𝑒 𝑅 𝐿 𝑡 . Multiplying this on both sides • 𝑒 𝑅 𝐿 𝑡 𝑑𝑖(𝑡) 𝑑𝑡 + 𝑒 𝑅 𝐿 𝑡 Ri(t) 𝐿 = 𝑒 𝑅 𝐿 𝑡 𝑉𝑠 𝐿 • 𝑑 (𝑒 𝑅 𝐿𝑡 ∗i t ) 𝑑𝑡 = 𝑒 𝑅 𝐿 𝑡 𝑉𝑠 𝐿 //Rewriting
  • 3. • 𝑑 (𝑒 𝑅 𝐿𝑡 ∗i t ) 𝑑𝑡 𝑑𝑡 = 𝑒 𝑅 𝐿 𝑡 𝑉𝑠 𝐿 𝑑𝑡 //Integrating on both sides • 𝑒 𝑅 𝐿 𝑡 ∗ i t = 𝑉𝑠 𝐿 𝑒 𝑅 𝐿 𝑡 ∗ 𝐿 𝑅 + 𝐾 => i t = 𝑉𝑠 𝑅 + 𝐾𝑒− 𝑅 𝐿 𝑡 • Applying initial condition at t=t0; i(t)=I0 • 𝐾 = 𝐼0 − 𝑉𝑠 𝑅 𝑒 𝑅 𝐿 𝑡0 • Substituting in i(t) • i t = 𝑉𝑠 𝑅 − 𝑉𝑠 𝑅 −𝐼0 𝑒− 𝑅 𝐿 (𝑡−𝑡0) If t=0; I0 =0 𝐢 𝐭 = 𝑽𝒔 𝑹 𝟏 − 𝒆− 𝑹𝒕 𝑳 𝒗𝑳 𝐭 = 𝐋 𝒅𝒊 𝒅𝒕 = 𝑽𝒔𝒆− 𝑹𝒕 𝑳
  • 4. Charging of a capacitor • 𝑉 𝑠 − 𝑅C 𝑑 𝑉𝑐 𝑡 𝑑𝑡 − Vc(t) = 0 • Rearranging • d𝑉𝑐(𝑡) dt + 𝑉𝑐 t RC = 𝑉𝑠 RC ; it is of the form 𝑑𝑦 𝑑𝑥 + p x ∗ y = q(x) • Integrating factor 𝑒 𝑃 𝑥 𝑑𝑥 = 𝑒 1 𝑅𝐶 𝑑𝑡 = 𝑒 1 𝑅𝐶 𝑡 . Multiplying this on both sides • 𝑒 1 𝑅𝐶 𝑡 d𝑉𝑐 t dt + 𝑒 1 𝑅𝐶 𝑡 𝑉𝑐 t RC = 𝑒 1 𝑅𝐶 𝑡 𝑉𝑠 RC • 𝑑 (𝑒 1 𝑅𝐶𝑡 ∗𝑉𝑐 t ) 𝑑𝑡 = 𝑒 1 𝑅𝐶 𝑡 𝑉𝑠 RC
  • 5. • Integrating on both sides • 𝑑 (𝑒 1 𝑅𝐶𝑡 ∗𝑽𝒄 𝐭 ) 𝑑𝑡 = 𝑒 1 𝑅𝐶 𝑡 𝑉𝑠 RC • 𝑒 1 𝑅𝐶 𝑡 ∗ 𝑽𝒄 𝐭 = 𝑒 1 𝑅𝐶 𝑡 𝑉 𝑠 + 𝐾 • 𝑽𝒄 𝐭 = 𝑉 𝑠 + 𝐾𝑒− 1 𝑅𝐶 𝑡 • Applying initial condition at t=t0; Vc(t)=V0 • 𝐾 = (𝑉0 − 𝑉𝑆)𝑒 1 𝑅𝐶 𝑡0 • Substituting in 𝑽𝒄 𝐭 • 𝑽𝒄 𝐭 = 𝑽𝒔 − (𝑽𝑺 − 𝑽𝟎)𝒆− 𝟏 𝑹𝑪 (𝒕−𝒕𝟎) If t=0; V0 =0 𝑽𝒄 𝐭 = 𝑽𝒔(𝟏 − 𝒆− 𝒕 𝑹𝑪) 𝒊 𝐭 = 𝑪 𝒅𝑽𝒄 𝐭 𝒅𝒕 = 𝑽𝒔 𝑹 𝒆− 𝒕 𝑹𝑪
  • 6. • If a given circuit is not in the form of standard RL/RC circuit. It can be converted to its thevenin’s equivalent across the inductor/capacitor. Eg Numerical 6) • For the circuit shown in figure below, the switch S has been closed for a long time and then opens at t = 0. Find, i. vab(0− ) ii. ix 0− iii. iL 0− iv. ix(0+ ) v. vab(0+ ) vi. ix(t = ∞) vii. vab(t = ∞) viii.ix t , for t > 0
  • 7. Solution: There is a current (I0) flowing in the inductor before switch is opened. To determine I0, Analyze the circuit before the switch is operated. 𝐢 𝐭 = 𝑽𝒔 𝑹 𝟏 − 𝒆− 𝑹𝒕 𝑳 𝑽𝒔=Vth=12.857 R=Rth=2.142Ω 𝐢 𝐭 = 𝟏𝟐. 𝟖𝟓𝟕𝟏 𝟐. 𝟏𝟒𝟐 𝟏 − 𝒆− 𝟐.𝟏𝟒𝟐𝒕 𝟏 = 𝟔 𝟏 − 𝒆− 𝟐.𝟏𝟒𝟐𝒕 𝟏 1 0  6  5  1 H 2 0 V a b i x 5  2 0 V a b 1 0  i x Since the switch is closed for a long time. Inductor behaves as a short circuit carrying a current 6A. i. vab 0− ⇒ 0. Behaves as a short circuit ii. ix 0− ⇒ 6 ∗ 10 15 = 4𝐴 iii. iL 0− ⇒ 6𝐴
  • 8. 10 6 5 1H 20V a b ix 𝐢 𝐭 = 𝑽𝒔 𝑹 − 𝑽𝒔 𝑹 −𝑰𝟎 𝒆− 𝑹 𝑳 (𝒕−𝒕𝟎) t0 = 0 I0=6A Vs=Vth=20V R=Rth=5Ω 𝐢 𝐭 = 𝟐𝟎 𝟓 − 𝟐𝟎 𝟓 − 𝟔 𝒆− 𝟓 𝟏 (𝒕−𝟎) 𝐢 𝐭 = 𝟒 − 𝟒 − 𝟔 𝒆−𝟓𝒕 𝐢 𝐭 = 𝟒 + 𝟐𝒆−𝟓𝒕 iv. ix 0 + ⇒ 𝑖𝐿 0 + = 6𝐴 v. vab(0+ ) ⇒ 20 − 5𝑖𝐿 0 + − 𝑉𝑎𝑏 = 0 ⇒ Vab = −10V vi. ix(t = ∞) ⇒ 𝑖𝐿 ∞ = 4𝐴 vii. vab t = ∞ = 0V. Inductor behaves as a short Before the switch is opened the current would reach a maximum of 6A . Therefore I0=6A For t>0
  • 9. Numerical 7) For the circuit shown in figure below, the switch S has been kept open for a long time and then it is closed at t = 0. Find, i. vc(0− ) ii. vc 0+ iii. ic 0− iv. ic(0+ ) v. dvc dt t=0+ vi. vc t = ∞ vii. find the time constants of the circuit before and after the switch is closed
  • 10. 1 0  4 0 V 4 F before the switch is operated 𝐕𝐜 𝐭 = 𝑽𝒔 𝟏 − 𝒆− 𝟏 𝑹𝑪 𝒕 Vc t = 40 1 − 𝑒− 1 40 𝑡 Capacitor is charged to a maximum of 40 V before the switch is operated. Hence behaves as an open circuit. vc 0− = 40V; ic 0− = 0A 𝝉1 = 40s After the switch is operated 𝐕𝐜 𝐭 = 𝑽𝒔 − (𝑽𝑺 − 𝑽𝟎)𝒆− 𝟏 𝑹𝑪 (𝒕−𝒕𝟎) Vs=Vth=15V R=Rth= 3.75Ω Vc t = 15 − 15 − 40 𝑒− 1 15 𝑡−0 Vc t = 15 + 25 𝑒− 1 15𝑡 vc 0+ = 40V; vc ∞ = 15V; 𝝉2 = 15s 1 0  4 0 V 4 F 6  𝑑Vc 0+ 𝑑𝑡 = − 5 3 𝐶 𝑑Vc 0+ 𝑑𝑡 = − 20 3
  • 11. Numerical 8) For the circuit shown below, switch S is kept in position ‘1’ for a long time and then it is moved to position ‘2’ at time 𝑡 = 0 . Find i. The current expression for 𝐢 𝐭 for 𝑡 ≥ 0 ii. Calculate the time constants of the circuit before and after the switching phases
  • 12. 10 25V 5 10 2 10 5A 5 10 2 Solution Switch in position 1 𝐕𝐜 𝐭 = 𝑽𝒔 𝟏 − 𝒆− 𝟏 𝑹𝑪 𝒕 Vs=Vth=10V R=Rth=6Ω 𝝉1= R*C=12µ 𝑽𝒄 𝒕 = 𝟏𝟎 𝟏 − 𝒆 − 𝟏 𝟏𝟐µ𝒕
  • 13. 10 30V 10 2 Switch in position 2 𝐕𝐜 𝐭 = 𝑽𝒔 − (𝑽𝑺 − 𝑽𝟎)𝒆− 𝟏 𝑹𝑪 (𝒕−𝒕𝟎) Vs=Vth=15V R=Rth= 5Ω 𝝉2= R*C=10µ Vc t = 15 − 15 − 10 𝑒 − 1 10µ 𝑡−0 𝑽𝒄 𝒕 = 𝟏𝟓 − 𝟓𝒆 − 𝟏 𝟏𝟎µ 𝒕 𝑖𝑐 = 𝐶 d𝑉𝑐(𝑡) dt = 2µ ∗ −5𝑒 − 1 10µ 𝑡 ∗ − 1 10µ = 𝑒 − 1 10µ 𝑡 𝑖10 = Vc t 10 = 1.5 − 0.5𝑒 − 1 10µ 𝑡 𝒊𝑿 = 𝟏. 𝟓 + 𝟎. 𝟓𝒆 − 𝟏 𝟏𝟎µ 𝒕