Op amp integrator

src: i.ytimg.com

The operational amplifier integrator is an electronic integration circuit. Based on the operational amplifier (op-amp), it performs the mathematical operation of integration with respect to time; that is, its output voltage is proportional to the input voltage integrated over time..

Video Op amp integrator

Applications

The integrator circuit is mostly used in analog computers, analog-to-digital converters and wave-shaping circuits. A common wave-shaping use is as a charge amplifier and they are usually constructed using an operational amplifier though they can use high gain discrete transistor configurations.

Maps Op amp integrator

Design

The input current is offset by a negative feedback current flowing in the capacitor, which is generated by an increase in output voltage of the amplifier. The output voltage is therefore dependent on the value of input current it has to offset and the inverse of the value of the feedback capacitor. The greater the capacitor value, the less output voltage has to be generated to produce a particular feedback current flow.

The input impedance of the circuit is almost zero because of the Miller effect. Hence all the stray capacitances (the cable capacitance, the amplifier input capacitance, etc.) are virtually grounded and they have no influence on the output signal.

Ideal circuit

The circuit operates by passing a current that charges or discharges the capacitor C_f during the time under consideration, which strives to retain the virtual ground condition at the input by off-setting the effect of the input current. Referring to the above diagram, if the op-amp is assumed to be ideal, nodes v₁ and v₂ are held equal, and so v₂ is a virtual ground. The input voltage passes a current ${\displaystyle {\frac {v_{in}}{R_{1}}}}$ through the resistor producing a compensating current flow through the series capacitor to maintain the virtual ground. This charges or discharges the capacitor over time. Because the resistor and capacitor are connected to a virtual ground, the input current does not vary with capacitor charge and a linear integration of output is achieved.

The circuit can be analyzed by applying Kirchhoff's current law at the node v₂, keeping ideal op-amp behaviour in mind.

${\displaystyle i_{\text{1}}=I_{\text{B}}+i_{\text{F}}}$

${\displaystyle I_{\text{B}}=0}$ in an ideal op-amp, so:

${\displaystyle i_{\text{1}}=i_{\text{F}}}$

Furthermore, the capacitor has a voltage-current relationship governed by the equation:

${\displaystyle I_{\text{C}}=C{\frac {dV_{\text{c}}}{dt}}}$

Substituting the appropriate variables:

${\displaystyle {\frac {v_{\text{in}}-v_{\text{2}}}{R_{\text{1}}}}=C_{\text{F}}{\frac {d(v_{\text{2}}-v_{\text{o}})}{dt}}}$

${\displaystyle v_{2}=v_{1}=0}$ in an ideal op-amp, resulting in:

${\displaystyle {\frac {v_{\text{in}}}{R_{\text{1}}}}=-C_{\text{F}}{\frac {dv_{\text{o}}}{dt}}}$

Integrating both sides with respect to time:

${\displaystyle \int _{0}^{t}{\frac {v_{\text{in}}}{R_{\text{1}}}}\ dt\ =-\int _{0}^{t}C_{\text{F}}{\frac {dv_{\text{o}}}{dt}}\,dt}$

If the initial value of v_o is assumed to be 0 V, this results in a DC error of:

${\displaystyle v_{\text{o}}=-{\frac {1}{R_{\text{1}}C_{\text{F}}}}\int _{0}^{t}v_{\text{in}}\,dt}$

Practical circuit

The ideal circuit is not a practical integrator design for a number of reasons. Practical op-amps have a finite open-loop gain, an input offset voltage and input bias currents (${\displaystyle I_{B}}$). This can cause several issues for the ideal design; most importantly, if ${\displaystyle v_{\text{in}}=0}$, both the output offset voltage and the input bias current ${\displaystyle I_{B}}$ can cause current to pass through the capacitor, causing the output voltage to drift over time until the op-amp saturates. Similarly, if ${\displaystyle v_{\text{in}}}$ were a signal centered about zero volts (i.e. without a DC component), no drift would be expected in an ideal circuit, but may occur in a real circuit. To negate the effect of the input bias current, it is necessary to set:

${\displaystyle R_{\text{on}}=R_{1}||R_{f}||R_{L}}$. The error voltage then becomes:

${\displaystyle V_{\text{E}}=\left({\frac {R_{\text{f}}}{R_{1}}}+1\right)V_{IOS}}$

The input bias current thus causes the same voltage drops at both the positive and negative terminals.

Also, in a DC steady state, the capacitor acts as an open circuit. The DC gain of the ideal circuit is therefore infinite (or in practice, the open-loop gain of a non-ideal op-amp). To counter this, a large resistor ${\displaystyle R_{F}}$ is inserted in parallel with the feedback capacitor, as shown in the figure above. This limits the DC gain of the circuit to a finite value, and hence changes the output drift into a finite, preferably small, DC error. Referring to the above diagram:

${\displaystyle V_{\text{E}}=\left({\frac {R_{\text{f}}}{R_{1}}}+1\right)\left(V_{IOS}+I_{BI}\left(R_{\text{f}}\parallel R_{1}\right)\right)}$

where ${\displaystyle V_{IOS}}$ is the input offset voltage and ${\displaystyle I_{BI}}$ is the input bias current on the inverting terminal. ${\displaystyle R_{f}\parallel R_{1}}$ indicates two resistance values in parallel.

src: i.stack.imgur.com

Frequency response

The frequency responses of the practical and ideal integrator are shown in the above figure. For both circuits, the crossover frequency ${\displaystyle f_{\text{b}}}$, at which the gain is 0 dB, is given by:

${\displaystyle f_{\text{b}}={\frac {1}{{2\pi }{R_{\text{1}}}{C_{\text{F}}}}}}$

The 3 dB cutoff frequency ${\displaystyle f_{\text{a}}}$ of the practical circuit is given by:

${\displaystyle f_{\text{a}}={\frac {1}{{2\pi }{R_{\text{F}}}{C_{\text{F}}}}}}$

The practical integrator circuit is equivalent to an active first-order low-pass filter. The gain is relatively constant up to the cutoff frequency and decreases by 20 dB per decade beyond it. The integration operation occurs for frequencies in the range ${\displaystyle \left[f_{\text{a}},f_{\text{b}}\right]}$, provided that ${\displaystyle f_{\text{a}}<f_{\text{b}}}$. This condition can be achieved by appropriate choice of ${\displaystyle R_{\text{F}}C_{\text{F}}}$ and ${\displaystyle R_{1}C_{\text{F}}}$ time constants.

src: i.ytimg.com

References

Source of the article : Wikipedia