# Charge amplifier

A charge amplifier is an electronic current integrator that produces a voltage output proportional to the integrated value of the input current. This is effectively a measurement of the electrical input charge; hence the naming of the device.

The amplifier offsets the input charge using a feedback reference capacitor, and produces an output voltage inversely proportional to the value of the reference capacitor but proportional to the total input charge flowing during the specified time period; hence the circuit acts as a charge-to-voltage converter. The gain of the circuit depends on the values of the feedback capacitor and the feed-in resistor.

## Design

Charge amplifiers are usually constructed using an operational amplifier or other high gain semiconductor circuit with a negative feedback capacitor. 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.[1]

### Ideal circuit

An "ideal circuit" for analysing charge amplifier operation is shown below:

The circuit operates by passing a current that charges or discharges the capacitor Cf 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 vo is assumed to be 0 V, this results in a DC error of:[2]

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

### 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:

${\displaystyle R_{\text{on}}=R_{1}||R_{f}}$.

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. A practical circuit is shown below.

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.

In practice, the gain of the circuit is expressed in charge input required to obtain a voltage output, such as picocoulomb per volt.

## Applications

Common applications include amplification of signals from such as piezoelectric sensors and photodiodes, in which the charge output from the transducer is converted into a voltage.

Charge amplifiers are also used extensively in instruments measuring ionizing radiation, such as the proportional counter or the scintillation counter, where the energy of each pulse of detected radiation due to an ionising event must be measured. Integrating the charge pulses from the detector gives a translation of input pulse energy to a peak voltage output, which can then be measured for each pulse. Normally this then goes to discrimination circuits or a multi channel analyzer.

Charge amplifiers are also used in the readout circuitry of CCD imagers and flat-panel X-ray detector arrays. The amplifier is able to convert the very small charge stored within an in-pixel capacitor to a voltage level that can be easily processed.

• Enables quasi-static measurements in certain situations, such as constant pressures on a piezo lasting several minutes[3]
• Piezo element transducer can be used in much hotter environments than those with internal electronics[3]
• Gain is dependent only on the feedback capacitor, unlike voltage amplifiers, which are affected greatly by the input capacitance of the amplifier and the parallel capacitance of the cable[3][4]

### Other uses

4. ^ "Maximum cable length for charge-mode piezoelectric accelerometers". Endevco. Jan. Retrieved 2007-10-26. Check date values in: |date= (help)