15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients...

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15: Transients (A) 15: Transients (A) Differential Equation Piecewise steady state inputs Step Input Negative exponentials Exponential Time Delays Inductor Transients Linearity Transient Amplitude Capacitor Voltage Continuity Summary E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 1 / 11

Transcript of 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients...

Page 1: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

15: Transients (A)

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 1 / 11

Page 2: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):

Page 3: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysis

Page 4: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysis

Page 5: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

Page 6: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt

Page 7: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR

Page 8: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR ⇒ RC dy

dt + y = x

Page 9: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR ⇒ RC dy

dt + y = x

General Solution: Particular Integral + Complementary Function

Page 10: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR ⇒ RC dy

dt + y = x

General Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to RC dydt + y = x

Page 11: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR ⇒ RC dy

dt + y = x

General Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to RC dydt + y = x

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution for y(t).

Page 12: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR ⇒ RC dy

dt + y = x

General Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to RC dydt + y = x

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution for y(t).

Complementary Function: Solution to RC dydt + y = 0

Page 13: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR ⇒ RC dy

dt + y = x

General Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to RC dydt + y = x

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution for y(t).

Complementary Function: Solution to RC dydt + y = 0

Does not depend on x(t), only on the circuit.

Page 14: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR ⇒ RC dy

dt + y = x

General Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to RC dydt + y = x

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution for y(t).

Complementary Function: Solution to RC dydt + y = 0

Does not depend on x(t), only on the circuit.Solution is y(t) = Ae−

t/τ

where τ = RC is the time constant of the circuit.

Page 15: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Differential Equation

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 2 / 11

To find y(t):x(t) constant: Nodal analysisx(t) sinusoidal: Phasors + nodal analysisx(t) anything else: Differential equation

i(t) = C dydt =

x−yR ⇒ RC dy

dt + y = x

General Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to RC dydt + y = x

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution for y(t).

Complementary Function: Solution to RC dydt + y = 0

Does not depend on x(t), only on the circuit.Solution is y(t) = Ae−

t/τ

where τ = RC is the time constant of the circuit.

The amplitude, A, is determined by the initial conditions at t = 0.

Page 16: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Piecewise steady state inputs

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 3 / 11

We will consider input signals that are sinusoidal or constant for a particulartime interval and then suddenly change in amplitude, phase or frequency.

Page 17: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Piecewise steady state inputs

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 3 / 11

We will consider input signals that are sinusoidal or constant for a particulartime interval and then suddenly change in amplitude, phase or frequency.

Output is the sum of the steady state and a transient:y(t) = ySS(t) + yTr(t)

Page 18: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Piecewise steady state inputs

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 3 / 11

We will consider input signals that are sinusoidal or constant for a particulartime interval and then suddenly change in amplitude, phase or frequency.

Output is the sum of the steady state and a transient:y(t) = ySS(t) + yTr(t)

Steady state, ySS(t), is the same frequency as theinput; use phasors + nodal analysis.

Page 19: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Piecewise steady state inputs

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 3 / 11

We will consider input signals that are sinusoidal or constant for a particulartime interval and then suddenly change in amplitude, phase or frequency.

Output is the sum of the steady state and a transient:y(t) = ySS(t) + yTr(t)

Steady state, ySS(t), is the same frequency as theinput; use phasors + nodal analysis.

Transient is always yTr(t) = Ae−t

τ at each change.

Page 20: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Piecewise steady state inputs

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 3 / 11

We will consider input signals that are sinusoidal or constant for a particulartime interval and then suddenly change in amplitude, phase or frequency.

Output is the sum of the steady state and a transient:y(t) = ySS(t) + yTr(t)

Steady state, ySS(t), is the same frequency as theinput; use phasors + nodal analysis.

Transient is always yTr(t) = Ae−t

τ at each change.

Page 21: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

-1 0 1 2 3

-2

0

2

4

t (ms)

Page 22: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

Page 23: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

Page 24: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

Steady State + Transienty(t) = ySS + yTr = 4 +Ae−

t/τ

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

Page 25: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

Steady State + Transienty(t) = ySS + yTr = 4 +Ae−

t/τ

To find A, use capacitor property:Capacitor voltage never changes abruptly

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

Page 26: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

Steady State + Transienty(t) = ySS + yTr = 4 +Ae−

t/τ

To find A, use capacitor property:Capacitor voltage never changes abruptly

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

y(0+) = 4 +A and y(0−) = 1

Page 27: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

Steady State + Transienty(t) = ySS + yTr = 4 +Ae−

t/τ

To find A, use capacitor property:Capacitor voltage never changes abruptly

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

y(0+) = 4 +A and y(0−) = 1⇒ 4 +A = 1

Page 28: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

Steady State + Transienty(t) = ySS + yTr = 4 +Ae−

t/τ

To find A, use capacitor property:Capacitor voltage never changes abruptly

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

y(0+) = 4 +A and y(0−) = 1⇒ 4 +A = 1⇒ A = −3

Page 29: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

Steady State + Transienty(t) = ySS + yTr = 4 +Ae−

t/τ

To find A, use capacitor property:Capacitor voltage never changes abruptly

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

yTr

y(0+) = 4 +A and y(0−) = 1⇒ 4 +A = 1⇒ A = −3

So transient: yTr(t) = −3e−t/τ

Page 30: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

Steady State + Transienty(t) = ySS + yTr = 4 +Ae−

t/τ

To find A, use capacitor property:Capacitor voltage never changes abruptly

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

yTr

y

y(0+) = 4 +A and y(0−) = 1⇒ 4 +A = 1⇒ A = −3

So transient: yTr(t) = −3e−t/τ and total y(t) = 4− 3e−t/τ

Page 31: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Step Input

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 4 / 11

For t < 0, y(t) = x(t) = 1For t ≥ 0, RC dy

dt + y = x= 4Time Const: τ = RC = 1ms

Steady State (Particular Integral)ySS(t) = x(t) = 4 for t ≥ 0

Transient (Complementary Function)yTr(t) = Ae−

t/τ

Steady State + Transienty(t) = ySS + yTr = 4 +Ae−

t/τ

To find A, use capacitor property:Capacitor voltage never changes abruptly

-1 0 1 2 3

-2

0

2

4

t (ms)

-1 0 1 2 3

-2

0

2

4

t (ms)

ySS

yTr

y

y(0+) = 4 +A and y(0−) = 1⇒ 4 +A = 1⇒ A = −3

So transient: yTr(t) = −3e−t/τ and total y(t) = 4− 3e−t/τ

Transient amplitude ⇐ capacitor voltage continuity: vC(0+) = vC(0−)

Page 32: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et

0 1 2 3 4 5

-10

0

10 et

t

Page 33: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4

0 1 2 3 4 5

-10

0

10 et3e¼t

t

Page 34: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Page 35: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t

0 2 4 6 8-2

0

22e-t

t

Page 36: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4

0 2 4 6 8-2

0

22e-t

e-¼t

t

Page 37: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4, −2e−t/2

0 2 4 6 8-2

0

22e-t

e-¼t

-2e-½t

t

Page 38: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4, −2e−t/2

Transients are negative exponentials.

0 2 4 6 8-2

0

22e-t

e-¼t

-2e-½t

t

Page 39: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4, −2e−t/2

Transients are negative exponentials.

0 2 4 6 8-2

0

22e-t

e-¼t

-2e-½t

t

Decay rate of e−t/a

a 2a 3a 4a 5a0

0.5

1

t

Page 40: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4, −2e−t/2

Transients are negative exponentials.

0 2 4 6 8-2

0

22e-t

e-¼t

-2e-½t

t

Decay rate of e−t/a

37% after 1 time constant

a 2a 3a 4a 5a0

0.5

1

0.37

t

Page 41: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4, −2e−t/2

Transients are negative exponentials.

0 2 4 6 8-2

0

22e-t

e-¼t

-2e-½t

t

Decay rate of e−t/a

37% after 1 time constant5% after 3

a 2a 3a 4a 5a0

0.5

1

0.37

0.05

t

Page 42: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4, −2e−t/2

Transients are negative exponentials.

0 2 4 6 8-2

0

22e-t

e-¼t

-2e-½t

t

Decay rate of e−t/a

37% after 1 time constant5% after 3, <1% after 5

a 2a 3a 4a 5a0

0.5

1

0.37

0.05 0.01

t

Page 43: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4, −2e−t/2

Transients are negative exponentials.

0 2 4 6 8-2

0

22e-t

e-¼t

-2e-½t

t

Decay rate of e−t/a

37% after 1 time constant5% after 3, <1% after 5

a 2a 3a 4a 5a0

0.5

1

0.37

0.05 0.01

t

Gradient of e−t/a

Gradient at t hits zero at t+ a.

a 2a 3a0

0.5

1

t

Page 44: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Negative exponentials

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 5 / 11

Positive exponentials grow to ±∞:et, 3et/4, −2et/2

0 1 2 3 4 5

-10

0

10 et3e¼t

-2e½t

t

Negative exponentials decay to 0:2e−t, e

−t/4, −2e−t/2

Transients are negative exponentials.

0 2 4 6 8-2

0

22e-t

e-¼t

-2e-½t

t

Decay rate of e−t/a

37% after 1 time constant5% after 3, <1% after 5

a 2a 3a 4a 5a0

0.5

1

0.37

0.05 0.01

t

Gradient of e−t/a

Gradient at t hits zero at t+ a.True for any t.

a 2a 3a0

0.5

1

t

Page 45: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Exponential Time Delays

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 6 / 11

Negative exponential with a finalvalue of F .

y(t) = F + (A− F ) e−(t−TA)/τ

Page 46: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Exponential Time Delays

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 6 / 11

Negative exponential with a finalvalue of F .

y(t) = F + (A− F ) e−(t−TA)/τ

How long does it take to go from A to B ?

Page 47: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Exponential Time Delays

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 6 / 11

Negative exponential with a finalvalue of F .

y(t) = F + (A− F ) e−(t−TA)/τ

How long does it take to go from A to B ?

At t = TB :y(TB) = B = F + (A− F ) e−(TB−TA)/τ

Page 48: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Exponential Time Delays

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 6 / 11

Negative exponential with a finalvalue of F .

y(t) = F + (A− F ) e−(t−TA)/τ

How long does it take to go from A to B ?

At t = TB :y(TB) = B = F + (A− F ) e−(TB−TA)/τ

B−FA−F = e

−(TB−TA)/τ

Page 49: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Exponential Time Delays

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 6 / 11

Negative exponential with a finalvalue of F .

y(t) = F + (A− F ) e−(t−TA)/τ

How long does it take to go from A to B ?

At t = TB :y(TB) = B = F + (A− F ) e−(TB−TA)/τ

B−FA−F = e

−(TB−TA)/τ

Hence TB − TA = τ ln(

A−FB−F

)

= τ ln(

initial distance toFfinal distance toF

)

Page 50: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Exponential Time Delays

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 6 / 11

Negative exponential with a finalvalue of F .

y(t) = F + (A− F ) e−(t−TA)/τ

How long does it take to go from A to B ?

At t = TB :y(TB) = B = F + (A− F ) e−(TB−TA)/τ

B−FA−F = e

−(TB−TA)/τ

Hence TB − TA = τ ln(

A−FB−F

)

= τ ln(

initial distance toFfinal distance toF

)

Useful formula - worth remembering.

Page 51: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

Page 52: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt

Page 53: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt

Page 54: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

Page 55: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Page 56: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Solution: Particular Integral + Complementary Function

Page 57: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to LR

dydt + y = L

Rdxdt

Page 58: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to LR

dydt + y = L

Rdxdt

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution, ySS(t).

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Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to LR

dydt + y = L

Rdxdt

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution, ySS(t).

Complementary Function: Solution to LR

dydt + y = 0

Page 60: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to LR

dydt + y = L

Rdxdt

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution, ySS(t).

Complementary Function: Solution to LR

dydt + y = 0

Does not depend on x(t), only on the circuit.

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Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to LR

dydt + y = L

Rdxdt

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution, ySS(t).

Complementary Function: Solution to LR

dydt + y = 0

Does not depend on x(t), only on the circuit.Solution is yTr(t) = Ae−

t/τ

where τ = LR is the time constant of the circuit.

Page 62: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to LR

dydt + y = L

Rdxdt

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution, ySS(t).

Complementary Function: Solution to LR

dydt + y = 0

Does not depend on x(t), only on the circuit.Solution is yTr(t) = Ae−

t/τ

where τ = LR is the time constant of the circuit.

1st order transient is always yTr(t) = Ae−t/τ where τ = RC or L

R

Page 63: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Inductor Transients

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 7 / 11

We know i = x−yR

y(t) = L didt =

LR ×

d(x−y)dt = L

Rdxdt − L

Rdydt

⇒ LR

dydt + y = L

Rdxdt

Solution: Particular Integral + Complementary Function

Particular Integral: Any solution to LR

dydt + y = L

Rdxdt

If x(t) is piecewise constant or sinusoidal, we will usenodal/phasor analysis to find the steady state solution, ySS(t).

Complementary Function: Solution to LR

dydt + y = 0

Does not depend on x(t), only on the circuit.Solution is yTr(t) = Ae−

t/τ

where τ = LR is the time constant of the circuit.

1st order transient is always yTr(t) = Ae−t/τ where τ = RC or L

RAmplitude A ⇐ no abrupt change in capacitor voltage or inductor current.

Page 64: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.

Page 65: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C .

Page 66: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Page 67: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Page 68: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Now v(t) = vSS(t) + vTr(t)= vSS(t) +Ae

−t/τ

Page 69: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Now v(t) = vSS(t) + vTr(t)= vSS(t) +Ae

−t/τ

Time constant is τ = RThC

where RTh is the Thévenin resistance.

Page 70: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Now v(t) = vSS(t) + vTr(t)= vSS(t) +Ae

−t/τ

Time constant is τ = RThC

where RTh is the Thévenin resistance.

Replace the capacitor with a voltage sourcev(t); all voltages and currents in the circuitwill remain unchanged.

Page 71: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Now v(t) = vSS(t) + vTr(t)= vSS(t) +Ae

−t/τ

Time constant is τ = RThC

where RTh is the Thévenin resistance.

Replace the capacitor with a voltage sourcev(t); all voltages and currents in the circuitwill remain unchanged.

Linearity: y = ax+ bv = ax+ bvSS + bvTr

Page 72: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Now v(t) = vSS(t) + vTr(t)= vSS(t) +Ae

−t/τ

Time constant is τ = RThC

where RTh is the Thévenin resistance.

Replace the capacitor with a voltage sourcev(t); all voltages and currents in the circuitwill remain unchanged.

Linearity: y = ax+ bv = ax+ bvSS + bvTr = ySS + bvTr

Page 73: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Now v(t) = vSS(t) + vTr(t)= vSS(t) +Ae

−t/τ

Time constant is τ = RThC

where RTh is the Thévenin resistance.

Replace the capacitor with a voltage sourcev(t); all voltages and currents in the circuitwill remain unchanged.

Linearity: y = ax+ bv = ax+ bvSS + bvTr = ySS + bvTr

All voltages and currents in a circuit have the same transient (but scaled).

Page 74: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Linearity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 8 / 11

1st order circuit has only one C or L.Make a Thévenin equivalent of the networkconnected to the terminals of C . Rememberx is a voltage source but y is not.

Now v(t) = vSS(t) + vTr(t)= vSS(t) +Ae

−t/τ

Time constant is τ = RThC

where RTh is the Thévenin resistance.

Replace the capacitor with a voltage sourcev(t); all voltages and currents in the circuitwill remain unchanged.

Linearity: y = ax+ bv = ax+ bvSS + bvTr = ySS + bvTr

All voltages and currents in a circuit have the same transient (but scaled).

The circuit’s time constant is τ = RThC or LRTh

where RTh is theThévenin resistance of the network connected to C or L.

Page 75: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)

Page 76: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

Page 77: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Page 78: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

Page 79: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+

Page 80: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1

Page 81: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Page 82: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Time Constant

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Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Time ConstantSet x ≡ 0 → RTh = 2k

Page 84: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Time ConstantSet x ≡ 0 → RTh = 2kτ = L

RTh= 2µs

Page 85: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Time ConstantSet x ≡ 0 → RTh = 2kτ = L

RTh= 2µs

Result

Page 86: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Time ConstantSet x ≡ 0 → RTh = 2kτ = L

RTh= 2µs

Resulty = ySS + (y (0+)− ySS (0+)) e−t/τ

Page 87: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Time ConstantSet x ≡ 0 → RTh = 2kτ = L

RTh= 2µs

Resulty = ySS + (y (0+)− ySS (0+)) e−t/τ

= 3 + (5− 3) e−t/τ

Page 88: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Time ConstantSet x ≡ 0 → RTh = 2kτ = L

RTh= 2µs

Resulty = ySS + (y (0+)− ySS (0+)) e−t/τ

= 3 + (5− 3) e−t/τ

= 3 + 2e−t/τ

Page 89: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Transient Amplitude

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 9 / 11

Find Steady State (DC ⇒ ZL = 0)Potential divider: ySS = 1

2x

ySS(0−) = 1, ySS(0+) = 3

Inductor Current ContinuityiSS(0−) = 1mA ⇒ iL(0+) = 1mA

At t = 0+x− y = 1mA× 1 k = 1y(0+) = x(0+)− 1 = 5

Time ConstantSet x ≡ 0 → RTh = 2kτ = L

RTh= 2µs

Resulty = ySS + (y (0+)− ySS (0+)) e−t/τ

= 3 + (5− 3) e−t/τ

= 3 + 2e−t/τ

Page 90: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

Page 91: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

Page 92: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

Page 93: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

ySS

Page 94: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

ySS

Page 95: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

At t = 0+: x = 4 and v = −3

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

ySS

Page 96: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

At t = 0+: x = 4 and v = −3KCL @ Y: y−(−3)

2R + y−46R = 0 -RC 0 RC 2RC 3RC

-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

ySS

Page 97: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

At t = 0+: x = 4 and v = −3KCL @ Y: y−(−3)

2R + y−46R = 0

y(0+) = −9+44 = − 5

4

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

ySS

Page 98: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

At t = 0+: x = 4 and v = −3KCL @ Y: y−(−3)

2R + y−46R = 0

y(0+) = −9+44 = − 5

4

Time Constantτ = RThC = 2RC (from earlier slide)

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

ySS

Page 99: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

At t = 0+: x = 4 and v = −3KCL @ Y: y−(−3)

2R + y−46R = 0

y(0+) = −9+44 = − 5

4

Time Constantτ = RThC = 2RC (from earlier slide)

Resulty = ySS + (y (0+)− ySS (0+)) e−t/τ

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

ySS

Page 100: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

At t = 0+: x = 4 and v = −3KCL @ Y: y−(−3)

2R + y−46R = 0

y(0+) = −9+44 = − 5

4

Time Constantτ = RThC = 2RC (from earlier slide)

Resulty = ySS + (y (0+)− ySS (0+)) e−t/τ

= 134 +

(

− 54 − 13

4

)

e−t/τ

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

ySS

Page 101: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

At t = 0+: x = 4 and v = −3KCL @ Y: y−(−3)

2R + y−46R = 0

y(0+) = −9+44 = − 5

4

Time Constantτ = RThC = 2RC (from earlier slide)

Resulty = ySS + (y (0+)− ySS (0+)) e−t/τ

= 134 +

(

− 54 − 13

4

)

e−t/τ

= 134 − 18

4 e−t/τ = 3 1

4 − 4 12e

−t/2RC

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

yTr

ySS

Page 102: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Capacitor Voltage Continuity

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 10 / 11

Find Steady State (DC ⇒ ZC = ∞)KCL @ V: v−x

4R + v8R + v−y

2R = 0

KCL @ Y: y−v2R + y−x

6R = 0

vSS = 34x, ySS = 13

16x

Capacitor Voltage ContinuityvSS(0−) = −3 ⇒ v(0+) = −3

At t = 0+: x = 4 and v = −3KCL @ Y: y−(−3)

2R + y−46R = 0

y(0+) = −9+44 = − 5

4

Time Constantτ = RThC = 2RC (from earlier slide)

Resulty = ySS + (y (0+)− ySS (0+)) e−t/τ

= 134 +

(

− 54 − 13

4

)

e−t/τ

= 134 − 18

4 e−t/τ = 3 1

4 − 4 12e

−t/2RC

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

-RC 0 RC 2RC 3RC-4

-2

0

2

4

t

yTr

ySS

y

Page 103: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Summary

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 11 / 11

• 1st order circuits: include one C or one L.◦ vC or iL never change abruptly. The output, y, is not necessarily

continuous unless it equals vC .

Page 104: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Summary

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 11 / 11

• 1st order circuits: include one C or one L.◦ vC or iL never change abruptly. The output, y, is not necessarily

continuous unless it equals vC .

• Circuit time constant: τ = RThC or LRTh

◦ RTh is the Thévenin resistance seen by C or L.◦ Same τ for all voltages and currents.

Page 105: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Summary

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 11 / 11

• 1st order circuits: include one C or one L.◦ vC or iL never change abruptly. The output, y, is not necessarily

continuous unless it equals vC .

• Circuit time constant: τ = RThC or LRTh

◦ RTh is the Thévenin resistance seen by C or L.◦ Same τ for all voltages and currents.

• Output = Steady State + Transient◦ Steady State: use nodal/Phasor analysis when input is piecewise

constant or piecewise sinusoidal. The steady state has the samefrequency as the input signal.

Page 106: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Summary

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 11 / 11

• 1st order circuits: include one C or one L.◦ vC or iL never change abruptly. The output, y, is not necessarily

continuous unless it equals vC .

• Circuit time constant: τ = RThC or LRTh

◦ RTh is the Thévenin resistance seen by C or L.◦ Same τ for all voltages and currents.

• Output = Steady State + Transient◦ Steady State: use nodal/Phasor analysis when input is piecewise

constant or piecewise sinusoidal. The steady state has the samefrequency as the input signal.

◦ Transient: Find vC(0−) or iL(0−): unchanged at t = 0+Find y(0+) assuming source of vC(0+) or iL(0+)Amplitude never complex, never depends on t.

Page 107: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Summary

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 11 / 11

• 1st order circuits: include one C or one L.◦ vC or iL never change abruptly. The output, y, is not necessarily

continuous unless it equals vC .

• Circuit time constant: τ = RThC or LRTh

◦ RTh is the Thévenin resistance seen by C or L.◦ Same τ for all voltages and currents.

• Output = Steady State + Transient◦ Steady State: use nodal/Phasor analysis when input is piecewise

constant or piecewise sinusoidal. The steady state has the samefrequency as the input signal.

◦ Transient: Find vC(0−) or iL(0−): unchanged at t = 0+Find y(0+) assuming source of vC(0+) or iL(0+)Amplitude never complex, never depends on t.

◦ y(t) = ySS(t) + (y(0+)− ySS(0+)) e−t/τ

Page 108: 15: Transients (A) - Imperial College London · 2017-09-13 · 15: Transients (A) 15: Transients (A) •Differential Equation •Piecewise steady state inputs •Step Input •Negative

Summary

15: Transients (A)

• Differential Equation

• Piecewise steady stateinputs

• Step Input

• Negative exponentials

• Exponential Time Delays

• Inductor Transients

• Linearity

• Transient Amplitude

• Capacitor VoltageContinuity

• Summary

E1.1 Analysis of Circuits (2017-10110) Transients (A): 15 – 11 / 11

• 1st order circuits: include one C or one L.◦ vC or iL never change abruptly. The output, y, is not necessarily

continuous unless it equals vC .

• Circuit time constant: τ = RThC or LRTh

◦ RTh is the Thévenin resistance seen by C or L.◦ Same τ for all voltages and currents.

• Output = Steady State + Transient◦ Steady State: use nodal/Phasor analysis when input is piecewise

constant or piecewise sinusoidal. The steady state has the samefrequency as the input signal.

◦ Transient: Find vC(0−) or iL(0−): unchanged at t = 0+Find y(0+) assuming source of vC(0+) or iL(0+)Amplitude never complex, never depends on t.

◦ y(t) = ySS(t) + (y(0+)− ySS(0+)) e−t/τ

See Hayt Ch 8 or Irwin Ch 7.