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Chapter 6 Second-Order Circuit
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What is second-order circuit?
A second-order circuit is characterized by a second-order differential equation. It consists of resistors and the equivalent of two energy storage elements. Typical examples of second-order circuits: a) series RLC circuit, b) parallel RLC circuit, c) RL circuit, d) RC circuit
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Second-Order Circuit Zero-input Response
Second-Order Circuit Zero-state Response Second-Order Circuit Complete Response
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• Application: Filters
+ - u i E • Application: Filters –A lowpass filter with a sharper cutoff than can be obtained with an RC circuit.
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§6-1 Zero-input Response of the Series RLC Circuit
An understanding of the natural response of the series RLC circuit is a necessary background for future studies in filter design and communications networks. Assume: S(t=0) i Find :uc(t),i(t),uL(t)(t≥0)
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characteristic equation : 特征方程
In general, a quadratic characteristic equation has two roots:
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Four distinct possibilities:
Case A: If two real, unequal negative roots Case B: If two real, equal negative roots Case C: If two complex conjugate roots Case D: If two imaginary conjugate roots
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Zero-input Response of the Series RLC circuit
Special case: Uc(0)=U0, IL(0)=0 过阻尼 there are two real, unequal negative roots Overdamped Case
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According to Initial Conditions :
∴ S(t=0) i
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and
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S(t=0) Uo i i Uc(0)=U IL(0)=0 t O
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非振荡放电 (过阻尼Overdamped Case)
S(t=0) Uo i i Uc(0)=U IL(0)=0 t O 非振荡放电 (过阻尼Overdamped Case)
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Uc(0)=U0, IL(0)=0 (2) 临界阻尼 There are two real, equal roots
Critically damped Case According to the initial conditions: Uc(0)=U0, IL(0)=0
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Then t O Uo i
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Underdamped Case (3) 欠阻尼 then The roots may be written as:
there are two complex conjugate roots when then The roots may be written as:
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δ ω ω0 δ和ω决定衰减快慢
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∵
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i 欠阻尼 能量转换关系 0 < t < uC减小,i 增大 < t < - uC减小,i 减小
R L C + - 0 < t < uC减小,i 增大 < t < - R L C + - uC减小,i 减小 Uo i - < t < R L C + - |uC |增大,i 减小 O ωt 欠阻尼
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+ L C - u t U L C w ) 90 sin( = + \
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等幅振荡(无阻尼) Undamped Case ωt L C + -
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Note : (1) the behavior of such a network is captured by the idea of damping, which is the gradual loss of the initial stored energy. By adjusting the value of R , the response may be made undamped, overdamped, critically damped, or underdamped. S(t=0) i
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uC(t) (2)Oscillatory response is possible due to the presence of the two types of storage elements. Having both L and C allows the flow of energy back and forth between the two. overdamped response critically damped response underdamped response (R=0 Undamped Case)
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uC(t) critically damped response overdamped response underdamped response (3)The critically damped case is the borderline between the underdamped and overdamped cases and it decays the fastest.
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§6-2 Second-order Circuit Complete Response
The general second-order linear differential equation with a step function input has the form The complete response can be found by partitioning y(t) into forced and natural components:
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yN(t) --- general solution of the homogeneous equation (input set to zero),
∴ yF=A/ao yF(t) ---a particular solution of the equation Combining the forced and natural responses 全响应=零输入响应 + 零状态响应
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Example Multisim analysis of this circuit 0.5H t=0 600Ω/6KΩ i + _ 24V uc 0.1µF 1KΩ
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学习要求 能根据给定的电路列写二阶动态电路的输入输出方程; 根据已知条件确定求解微分方程的初始条件; 能根据电路参数定性地判断R、L、C串联电路的零输入响应的几种放电类型。
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Summary 1). 一阶电路是单调的响应,时间常数表示过渡过程的时间。 2). 二阶电路用三个参数 , 和 0来表示动态响应。满足:
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