Simple Three-Input Single-Output Current-Mode Universal Filter Using Single VDCC

International Journal of Electrical and Computer Engineering (IJECE)
Vol. 8, No. 6, December 2018, pp. 4932~4940
ISSN: 2088-8708, DOI: 10.11591/ijece.v8i6.pp4932-4940  4932
Journal homepage: http://iaescore.com/journals/index.php/IJECE
Simple Three-Input Single-Output Current-Mode Universal
Filter Using Single VDCC
Prungsak Uttaphut
Department of Electrical Technology, Faculty of Industrial Technology, Suan Sunandha Rajabhat University, Thailand
Article Info ABSTRACT
Article history:
Received Apr 1, 2018
Revised Jun 4, 2018
Accepted Jul 22, 2018
This paper presents a second-order current-mode filter with three-inputs and
single-output current using single voltage differencing current conveyors
(VDCC) along with one resistor and two grounded capacitors. The design of
presented filter emphasizes on the use of a single active element without the
multiple terminals VDCC which is convenient to implement the VDCC using
commercially available IC for the practical test. Also, it can reduce the
current tracking error at current output port and can reduce the number of
transistors in the VDCC. The proposed filter can realize all the five generic
filter responses, namely, band-pass (BP), band-reject (BR), low-pass (LP),
high-pass (HP), and all-pass (AP) functions from the same configuration
under various conditions in terms of three input current signals. Furthermore,
the natural frequency and quality factor are electronically controlled. The
output current node exhibits high impedance. Besides, the non-ideal case is
also investigated. The simulation and experimental results using VDCC
constructed from commercially available IC can validate the theoretical
analyses.
Keyword:
Active filter
commercially available IC
Electronic control
Universal biquad
VDCC
Copyright © 2018 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Prungsak Uttaphut,
Department of Electrical Technology, Faculty of Industrial Technology,
Suan Sunandha Rajabhat University,
1 U-Thong Nok Road, Dusit, Bangkok 10300, Thailand.
Email: prungsak.ssru@hotmail.com
1. INTRODUCTION
Analog filters are an important building blocks for analog signal processing that have a variety of
applications in the fields of communication, sound system, instrumentation, control system, etc [1]. The filter
which provides several filter responses in the same topology is well-known as the universal filter or
multifunction filter. The multifunction filter with multiple inputs and single output is one of the universal
filters which have attracted significant research attention [2]. In addition to these, a current-mode (CM)
signal processing circuits in which some parameters can be controlled by external currents have low power
consumption, greater linearity, a smaller number of components and larger dynamic range, wider bandwidth
when compared to voltage-mode counterparts such as operational amplifiers [3]-[4].
The design of an electronic circuit in analog signal processing has gone in the use of the active
building block [5]-[9]. Especially, the electronically tunable active building blocks have attracted significant
research attention since analog circuits using electronically tunable active building block give more fine-
tuning than adjusting the value of passive device. The voltage differencing current conveyors (VDCC) [10] is
a recently reported versatile active building block used in the realization of analog signal processing circuits.
A very significant advantage of using VDCCs in analog circuit design is that it is able
electronic controllability.
Analog circuits using the VDCC as the active element have been found in the literature for
examples, the first order allpass filter [11], the ladder filter [12], the passive element simulator [10], [13]-

Int J Elec & Comp Eng ISSN: 2088-8708 
Simple Three-Input Single-Output Current-Mode Universal Filter Using Single VDCC (Prungsak Uttaphut)
4933
[16], the square and triangular wave generator [17], sinusoidal oscillator [18]-[21], etc. The VDCC based
universal filters have been proposed in [22]-[25]. The three-input single-output (TISO) voltage-mode filter
and single-input dual-output (SIDO) voltage-mode filters were presented in [22]. The TISO filter with five
filter responses consists of single VDCC, one resistor and two capacitors. The SIDO filters with three filter
responses (HP, BP and LP) consist of single VDCC, two resistors and two capacitors. The natural frequency
and quality factor for both TISO and SIDO are electronically tuned. Moreover, the tune of quality factor for
SIDO filter can be done without affecting the natural frequency. However, the output voltage node doesn’t
exhibit low impedance, so the voltage buffer is required for cascading. The single-input four-output voltage-
mode filter was proposed in [23]. It consists of single VDCC, two resistors and two capacitors. The natural
frequency and quality factor are electronically tuned. Moreover, the tune of quality factor can be done
without affecting the natural frequency. However, the output voltage nodes don’t exhibit low impedance, so
the voltage buffer is required for cascading. The current-mode reconnection-less reconfigurable filter was
proposed in [24]. It consists of single VDCC, a single dual output current amplifier, a single resister and two
grounded capacitors. The natural frequency and quality factor are electronically tuned. The impedance at
input current node exhibits low and the impedance at output current node exhibits high which is convenient
to cascade in the current-mode circuit without the use of any current buffer. However, this filter can provide
only three filter responses (LP, HP and BP). Also, it requires the multiple output terminal active devices. The
three-input single-output current-mode universal filter with five filter responses was proposed in [25]. It
consists of single VDCC, a single grounded resister and two grounded capacitors. The natural frequency and
quality factor are electronically tuned. The impedance at the output current node exhibits high which is
convenient to cascade in the current-mode circuit without the use of any current buffer. However, this filter
requires the multiple output terminals of VDCC.
The three-input single-output current-mode biquad filter emphasizing on the use of the VDCC is
present in this paper. The proposed filter consists of single VDCC, one resistor and two grounded capacitors
which are suitable for the chip and off-the-shelf implementation. The natural frequency and quality factor can
be electronically adjusted. The simulation results of the proposed filter agree well with the theoretical
expectation.
2. THE PRINCIPLE OF OPERATION
2.1. Voltage differencing current conveyor (VDCC)
In this design, the active building block (ABB) called the voltage differencing current conveyor
(VDCC) is used as the main active device. The international construction of CMOS VDCC was proposed by
Firat et al [10] in 2014. It is five port device namely P, N, Z, X and W port. The high impedance voltage
input ports are P and N. The high impedance current output ports are Z and W port. The low impedance
voltage output port is X port. In the original version of VDCC, the output current at W port provides the
output current both positive and negative direction called Wn and Wp ports. For this purpose, a single W port
is required. This can reduce the current tracking error at W port and can reduce the number of transistor in
the VDCC. The electrical symbol and the equivalent circuit of the VDCC are shown in Figure 1 (a) and (b).
The ideal electrical properties of the VDCC are shown in equation (1).
0 0 0 0
0 0 0 0
0 0
0 0 1 0
0 0 0 1
N
P
P
N
Z m m
Z
X
X
W
I
V
I
V
I g g
V
V
I
I
   
    
    
    = −
    
     
   
  
(1)
where gm is the transconductance gain. The VDCC can be constructed from commercially available ICs as
shown in Figure 1(c). It consists of LM13700 [26] and AD844 [27]. This construction contains only the
single w terminal. The gm for this construction is given as
2
B
m
T
I
g
V
= (2)
where IB is DC bias current and VT is thermal voltage.

 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 8, No. 6, December 2018 : 4932 - 4940
4934
N
P
Z
WVDCC
PV
WI
ZI
zV
PI
NI
NV
XI
X
XV
BI
VDCC
Iw
VxVz
gm(VP - VN)VP
VN
Ix
1
IB
Ix
LM13700
AD844
( )m P Ng V V−
PV
NV
Z X
w
BI
mg+
−
VDCC
y
x
z
(a) (b) (c)
Figure 1. VDCC (a) Circuit symbol of VDCC (b) Equivalent circuit (c) VDCC (without the dual W terminal)
constructed from commercially available ICs
2.2. Proposed filter
The proposed filter is shown in Figure 2. It consists of single VDCC, one resistor and two grounded
capacitors. There are three input currents, ii1, ii2 and ii3. The single output current is iout which exhibits high
impedance at the current output node. It is found that the proposed filter doesn’t require VDCC with multiple
W terminals unlike the current-mode filter using VDCC as the active element presented in [24]-[25]. This
makes the VDCC used in the proposed filter is more convenient to construct by using commercially available
ICs. Routine analysis of the proposed filter using equation (1) yields the following output current equation
2
1 2 3
1 2 1 2 2 1 2
2
2 1 2
1 1 1
1
m m
i i i
out
m
g g
i s i s i s s
C R C R C C R C R C C R
i
g
s s
C R C C R
   
− + + + +   
   =
+ +
(3)
From equation (3), the natural frequency and qualigy factor are given as
0
1 2
mg
C C R
 = and 2
1
mC g R
Q
C
= (4)
It is evident from equation (4) that the natural frequency and quality factor can be electronically tuned via gm.
N
P
Z
WVDCC
X
BI
1C
R2ii
2C
1ii 3ii
outi
Figure 2. Proposed filter
From equation (3), the derivation of five filter responses can be done as follows:
• The non-inverting band-pass filter response can be obtained by applying the input current to ii1 while ii2
and ii3 being zero (no the input current applying).
• The non-inverting low-pass filter response can be obtained by applying the input current to ii1 and ii2
while ii3 being zero and C1=C2.
• The non-inverting high-pass filter response can be obtained by applying the input current to ii2 and ii3

4935
while ii1 being zero.
• The non-inverting band-reject filter response can be obtained by applying the input current to ii3 and
applying the inverting input current to ii1 while ii2 being zero.
• The non-inverting all-pass filter response can be obtained by applying the input current to ii3 and applying
the double inverting input current to ii1 while ii2 being zero.
3. NON-IDEAL ANALYSIS
In practically, the influent of current/voltage tracking errors and parasitic elements in the VDCC will
affect the performances of the proposed filter. For the non-ideal case, the relationship of the terminal voltages
and currents of the VDCC can be rewritten as:
0 0 0 0
0 0 0 0
0 0
0 0 0
0 0 0
N
P
P
N
Z m m
Z
X
X
W
I
V
I
V
I g g
V
V
I
I


   
    
    
    = −
    
     
   
   (5)
where  is the voltage tracking error from X to Z terminal and  is the current tracking error from X to W
terminal. The various ports of VDCC are characterized by parasitic resistances (RP, RN, RZ, RX and RW) and
parasitic capacitances (CP, CN, CZ, and CW) as shown in Figure 3(a). Taking parasitic elements in VDCC into
account, the proposed circuit in Figure 2 is re-drawn as shown in Figure 3(b). Taking the non-ideal
parameters into account, the output current of the circuit in Figure 2 is obtained as
( ) ( )1 2 2 1 3 1 2 1
3 1 2 1
'1
1 '
i i m i m
out
L m
i Y i Y g i YY R Y g
i
Y R YY R Y g
   

− + + + +  
=   
+ + +   (6)
where Y1 = s(C1+Cz)+Gz, Y2 = s(C1+CN)+GN, Y3 = sCW+ GW, R′ = R+Rx, and RL is the load resistance. If RL
is low and the operational frequency fop<<1/CWRW, the output current in equation (6) becomes
1 2' ' ' ' ' ' ' ' ' ' ' ' '
1 1 2 2 1 2 1 2
2
3 ' ' ' ' ' ' ' '
1 2 2 2 1 2
2
' ' ' ' ' '
1 2 2 2 1 2
1
1
N mz
i i
N N z z mz
i
out
N N z z mz
G gG
i s i s
C R C C R C R C C R C C R
G G G G gG
i s s
C C C C R C C R
i
G G G G gG
s s
C C C C R C C
  


    
+ − + + +    
    
 
   + + + + + +   
   =
  + +
+ + + + 
 
' '
R
(7)
From equation (7), the natural frequency is given as
( )( )( )0
1 2
N z z m
z N X
G G G g
C C C C R R


+ +
=
+ + +
(8)
Subsequently, the quality factor is given as
( )
( ) ( )( ) ( )
( )( )( )
( )
1 2
1 1 1
z N X N z z m
z X z X N z z
C C C C R R G G G g
Q
G R R C C R R G C C C C
 + + + + +
 = 
+ + + + + + +   (9)

 ISSN: 2088-8708
4936
N
P
Z
W
X
BI
ZC XR
NC
ZR
NR
PR PC
WC WR
VDCC
N
P
Z
WVDCC
X
BI
1Y
'R2ii
2Y
1ii
3ii
outi
LR3Y
(a) (b)
Figure 3. (a) Parasitic elements appeared in VDCC terminals (b) The proposed filter with parasitic elements
4. SIMULATION RESULTS
The simulation was done by using the LM13700 and AD844 PSPICE macro model parameters to
confirm the functionality of the proposed filter. The internal construction of the VDCC was constructed as
shown in Figure 2(c). The proposed circuit was supplied with symmetrical ±5 VDC, the DC bias current was
set as IB = 52 A and the passive component values were chosen as R = 1 kΩ and C1 = C2 = 1 nF. With
mentioned active and passive component values, the theoretical natural frequency and quality factor from
equation (4) are respectively obtained as f0 = 159.23 kHz, Q = 1.
The simulated gain for LP, HP, BP and BR versus frequency response of the proposed filter with
mentioned active and passive component values is shown in Figure 4. The simulated natural frequency is
154.88 kHz. The deviation of theoretical and simulated natural frequency is 2.73%. This deviation suffers
from the voltage/current tracking error and parasitic elements as analyzed in equation (8). The simulated gain
and phase of AP versus frequency response is shown in Figure 5. It is found that phase response changes
from 0 to -360 while the magnitude frequency response is constant for all frequencies. The results in Figure
4 and 5 confirm that the proposed circuit can provide five filter responses with the same circuit topology.
Frequency (Hz)
1.0k 10k 100k 1.0M 10M
-100
-50
0
20
Gain(dB)
HP
BP
LP
BR
Figure 4. Simulated gain response of the proposed filer
Frequency (Hz)
1.0k 10k 100k 1.0M 10M
-400d
-300d
-200d
-100d
0d
-10
-5
0
5
10
Gain(dB)
Phase
Gain
Phase
Figure 5. Simulated phase and gain response of all-pass function
The simulated input and output waveform in the time domain for the BP functions is illustrated in
Figure 6 when three frequencies, 10 kHz, 154.88 kHz and 1 MHz with 20 Ap-p were applied as input current.
It is found that the magnitude of output current has the highest amplitude at f=154.88 kHz. The tuning of
phase response for the AP function was tested as shown in Figure 7 by applying the input current as the
sinusoidal signal with 20 Ap-p and f=154.88 kHz while the DC bias current was adjusted for three values, 52
A, 90 A and 208 A. It is found that the phase response of AP function can be controllable with constant

4937
amplitude. THD analysis of the proposed current-mode universal filter given in Figure 8 was performed at
154.88 kHz for various sinusoidal peak input.
Time (µs)
0 50 100 150 200 250 300 350 400-10
-5
0
5
10
Current(µA)
iin
iout
(a)
Time (µs)
0 2 4 6 8 10 12 14 16 18 20 22 24
-
10
-5
0
5
10
Current(µA)
iout
iin
(b)
Time (µs)
0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0
-
10
-5
0
5
10
Current(µA)
iout
iin
(c)
Figure 6. The simulated waveforms of the BP filter at (a) 10 kHz (b) 154.88 kHz and (c) 1 MHz
Time (µs)
10 12 14 16 18 20 22 24 26 28 30 32 34 36
-12
0
12
Current(µA)
IB=52µA
IB=90µA
IB=208µA
Figure 7. The measured output waveforms of the all-pass filter for different IB values
iin (uAp)
0 20 40 60 80 100
THD(%)
0.0
.5
1.0
1.5
2.0
2.5
3.0
3.5
Figure 8. THD variation with respect to applied sinusoidal input current

 ISSN: 2088-8708
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5. EXPERIMENTAL RESULTS
The proposed filter in Figure 2 was experimentally tested using VDCC construced from the
LM13700 and AD844 commercially available ICs as inlustrated in Figure 1(c). The input currents were
converted from the input voltage signal by using the AD844 IC and one resistor as shown in Figure 9. The
1k resistor was used as the output load to convert the output current to be the output voltage. The LM13700
and AD844 were biased with a DC supply voltage of ±5V and bias current of IB = 52A. All capacitances
and resistance were given by 1 nF and 1 k, respectively. The amplitude of input voltage for this test was 50
mVp-p. The experimentally observed frequency response of the LP, HP, BP and BR filter is shown in Figure
10. The measured f0 was obtained around 160 kHz. The measurement of the input voltage and output voltage
dropped at the output resistance load for the BP response is shown in Figure 11. The experimentally
measured gain and phase response of the AP filter is illustrated in Figure 12. It is found that experimental
results are in well accordance to the theoretical analyses.
AD844
inv y
x
z
1k
Non-inverting
input current
ini AD844
inv
y
x
z
1k
Inverting
input current
ini−
AD844
inv y
x
z
0.5k
Non-inverting
double input
current
2 ini
Frequency (kHz)
1 10 100 1000 10000
Gain(dB)
-60
-40
-20
0
Ideal
Low-pass
High-pass
Band-pass
Band-reject
Figure 9. Implementation of input currents using
AD844
Figure 10. Experimental gain response of the
proposed filer
(a) (b)
(c)
Figure 11. The input and output waveforms of BP filter at (a) 10 kHz (b) 160 kHz and (c) 1 MHz.

4939
Frequency (kHz)
1 10 100 1000 10000
Phase(degree)
-400
-300
-200
-100
0
Gain(dB)
-20
-10
0
10
20
Phase (Ideal)
Phase (Experimental)
Gain (Ideal)
Gain (Exprimental)
Figure 12. Experimental phase and gain response of the all-pass function
6. CONCLUSION
In this contribution, the three-input single-output current-mode filter is presented. The proposed
filter uses only single VDCC as active element. The natural frequency and quality factor can be tuned
electronically by changing the bias current of VDCC. Using only VDCC constructed from commercially
available ICs, the proposed filter is suitable for off-the-shelf implementation. The workability of the proposed
filter is demonstrated by simulation and experimental results.
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