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Journal of Engineering

Volume 2013 (2013), Article ID 309124, 6 pages

http://dx.doi.org/10.1155/2013/309124

## Voltage Mode Pulse Width Modulator Using Single Operational Transresistance Amplifier

^{1}Department of Electronics and Communication, Delhi Technological University, Bawana Road, Delhi 110042, India^{2}Department of Electronics Engineering, Indian School of Mines, Dhanbad, Jharkhand 826004, India

Received 31 August 2012; Revised 2 December 2012; Accepted 10 December 2012

Academic Editor: Kyoung Kwan Ahn

Copyright © 2013 Rajeshwari Pandey et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

This paper presents a voltage mode pulse width modulator (PWM) using single operational transresistance amplifier (OTRA). The proposed PWM consists of a relaxation oscillator output which is modulated using modulating signal. PSPICE simulation results and experimental results have been included to verify the theoretical analysis.

#### 1. Introduction

Pulse width modulation (PWM) scheme is widely used in communication systems, DC motor speed controller, power conversion control circuits [1–3], and instrumentation. In PWM, the width of pulses of a pulse train is changed in accordance to voltage level of modulating signal. The PWM generators are available in Integrated Circuits (ICs) form; however, the internal circuitry is somewhat complex and typically consists of current sources, flip-flop, comparators, and analog switches [4]. Apart from these readily available ICs, the PWM signal can most commonly be generated by comparing a modulating signal with a sawtooth or triangular waveform. Alternatively, information signal can first be combined with a sawtooth or triangular waveform and thereafter comparing the combined signal with a reference level to generate PWM signal. This can be implemented using a Schmitt trigger with an RC circuit in feedback loop [5]. Extensive literature review reveals that PWMs based on this concept are available using different active analog building blocks such as op-amps [6], current conveyor II (CCII) [4], and operational transconductance amplifier (OTA) [7, 8]. High-frequency performance of PWMs employing op-amps is limited due to lower slew rate and constant gain-bandwidth product of the op-amps. The CCII-based PWM has the advantage of generating accurate PWM signal with high operating frequencies [4], and the output amplitude and frequency of the PWMs based on OTAs can be independently/electronically tuned [7]. Despite these advantages, the circuits proposed in [4, 7] suffer a drawback of using excessive number of active elements. Reference [8] presents another OTA-based PWM which uses derivative method. In derivative method, the duty cycle of PWM signal depends on a differentiated result of the modulating signal. This method is not suitable for applications where the changes in modulating signal are rare, such as in power converters [7]. The open literature suggests that a PWM pulse train can also be produced with the use of voltage-controlled delay lines [9], current-controlled delay cells [10], and voltage-controlled phase shifter [11] wherein the underlying concept is not the same as used in [4–8]; that is, the comparison of modulating signal with reference triangular/sawtooth waveform [9] uses two voltage-controlled delay lines, a fixed delay element, two rising edge detectors, along with an RS latch to generate a 0%–50% duty cycle at the output of the latch. Two 0%–50% modulators are connected in parallel to extend the duty cycle to 100%. Current-controlled delay cell-based duty oscillator and pseudohyperbola charge current generator are used in [10] for generating PWM. Yet, another PWM is proposed in [11] which employs a voltage-controlled phase shifter, a two-input logic AND gate, a network of logic inverters, and FET switches. This circuit generates a 0% to 50% pulse width using the phase shifter and an AND gate and then extends the range to 0%–100% using the inverters.

This paper aims at presenting an operational transresistance amplifier (OTRA) based PWM, using a relatively simpler scheme, wherein the modulating signal is combined with an exponential carrier waveform and compared with a reference. This paper is organized as follows. In Section 2, the function of an OTRA is briefly described, followed by the operation principle of the proposed PWM circuit. The feasibility of the presented circuits is verified through circuit simulations and experimental results in Section 3. It is observed that the simulation and experimental results are in close agreements with theoretical propositions. The comparison of the proposed circuit with earlier reported structures is presented in Section 4. Section 5 concludes the paper.

#### 2. Circuit Descriptions

OTRA is a high gain current input voltage output device. The input terminals of OTRA are internally grounded, thereby eliminating response limitations due to parasitic capacitances and resistances and, hence, are appropriate for high-frequency operation. The circuit symbol of OTRA is shown in Figure 1, and the port characteristics are given by (1), where is transresistance gain of OTRA. For ideal operations, the of OTRA approaches infinity and forces the input currents to be equal. Thus, OTRA must be used in a negative feedback configuration. Consider

The general scheme of PWM is depicted in Figure 2. The modulating signal and carrier signal are first summed up, and then PWM output signal is generated by comparing the summation signal and reference level.

The proposed PWM circuit is shown in Figure 3. The circuit consisting of OTRA, resistors and , and capacitor serves as square wave generator. Exponential voltage waveform across capacitor serves as carrier waveform. The modulating signal and the carrier wave are summed up at node through resistor . Thus, the voltage across the capacitor will be summation of carrier and modulating signal, and the PWM output is available at .

The resistor and capacitor form a positive feedback loop. and are the two possible saturation levels of output . Assume initially that switches to saturation level at , as shown in Figure 4. This results in charging of the capacitor present in the feedback loop, and the voltage across the capacitor reaches , a value at which , the current through terminal, becomes slightly less than the current through terminal, . As a result, the output voltage switches to , and the capacitor starts charging in the opposite direction. Now, as capacitor voltage approaches , the output once again switches back to .

The and values can be obtained from the routine analysis of this PWM circuit and are expressed by (2) and (3), respectively. Consider

These values of and result in and as follows: The overall period of the modulated output is given by and the duty factor () can be computed as

Equation (4) shows that the duty cycle of the output can be controlled with the help of modulating signal .

#### 3. Realizing an OTRA and Nonideality Analysis

For the proposed PWM circuit, the OTRA was realized using AD844 CFOA IC as shown in Figure 5 [12]. The equivalent circuit of Figure 5 for nonideal analysis [13] is presented in Figure 6. The CFOAs have been replaced with current conveyors having finite input resistances () and finite resistance at its terminal (). Ideally, the input resistance at the terminal is zero and is infinite at the terminal. For the AD844 CFOA, the input resistance is around 50 Ω, and is around 3 MΩ [14].

From Figure 6, various currents can be calculated as follows:

Ideally, should be equal to , which can be approximated only if , which is true for AD844. Also, the approximation that the input terminals are virtually grounded will be true only if the external resistance at the input terminal of the OTRA is much larger than . If these two conditions are satisfied, the OTRA constructed with AD844 closely approximates an ideal OTRA.

From (7), the output voltage , taking into account the previously mentioned approximations, can be calculated as where is the transimpedance gain of the OTRA.

If in PWM circuit shown in Figure 3 the equivalent circuit of OTRA constructed with AD844 is used, then the threshold limits of the output get modified to

The external resistance at the input of the OTRA should be much larger than R_{X} so that the feedback current can be absorbed into the input terminals. Since , , , and , Equations (9) and (10) reduce to (2) and (3), respectively.

#### 4. Simulation and Experimental Results

The proposed circuit is simulated using PSPICE. OTRA is realized using current feedback operational amplifiers (CFOAs) IC AD844 as shown in Figure 5. Macro model of AD844 is used for simulations. Figure7 shows the output voltage of the PWM when modulating signal is not applied, for KΩ, KΩ, KΩ, and pF, and corresponds to a 50% duty cycle. The observed output frequency is 66.7 KHz as against the calculated value of 69.7 KHz.

Simulated output of pulse width modulator, with same component values as used in Figure 7, is shown in Figure 8 for a 5 V, 1 KHz sinusoidal modulating signal. Figure 8(a) shows the modulating signal and the PWM output, and summation of modulating and carrier wave is depicted in Figure 8(b). Figures 9 and 10 show the output of pulse width modulator for an 8 V, 2.2 KHz modulating signal and 5 V, 40 KHz modulating signal, respectively, for same set of component values. Frequency spectrum of the pulse width modulator for 8 V, 2.2 KHz modulating signal is shown in Figure 11 which consists of modulating component and carrier signal. Thus, the modulating signal can be recovered with the help of appropriate low pass filter.

Figure 12 shows the variation of theoretically computed and simulated % duty factor of the modulator with the applied input signals. This shows that the two results closely match with each other.

The functionality of the proposed pulse width modulator circuits is verified through hardware as well.

The commercial IC AD844AN is used to implement an OTRA. Supply voltages used are ±5 V. Figure 13 shows typical experimental results of the circuit for two different modulating signals. Figure 13(a) depicts output for component values , , and and for an 8 V, 2.2 KHz modulating signal. Another screen shot of oscilloscope is shown in Figure 13(b) for a high-frequency modulating signal of 40 KHz with 5 V amplitude. These experimental results are in close agreement to simulated results.

#### 5. Comparison

In this section, a comparison of the proposed work with the previously reported analog PWM circuits [4, 6–8] is presented, which are all based on the concept of comparing a modulating signal with a reference sawtooth or triangular waveform to generate PWM signal. Table 1 shows the detailed comparison. The study of Table 1 reveals that topologies presented in [4, 7, 8] use more number of active components as compared to the proposed work. The proposed circuit is simpler as compared to the topologies of [4, 7, 8], since it uses the exponential voltage waveform across the capacitor of the square wave generator as carrier wave and, hence, does not require additional circuitry needed for triangular/sawtooth waves. Though exponential carrier wave being a nonlinear signal yields relatively inaccurate PWM signal at lower carrier frequencies as compared to the triangular/sawtooth wave, yet one can trade off accuracy for simplicity depending upon the application.

The PWM topology of [6], which is a classical opamp-based design, uses same number of active and passive components as in proposed circuit. However, the opamp-based circuits show limited high-frequency performance due to lower slew rate and constant gain-bandwidth product of the op-amps. Additionally, the input terminals of OTRA being virtually grounded, the proposed circuit is free from parasitic effects.

#### 6. Conclusion

In this paper, single OTRA-based PWM generator, a nonlinear application of OTRA, is proposed. This circuit can be used for speed control of DC motors and for DC-DC converters. PSPICE simulation results using AD844 macromodel and experimental results have been included for verification of the theoretical propositions which are found in close agreement.

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