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© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 510
Design of a Cell Charger for an iPad Using Full
Bridge Rectifier and Flyback Converter
1
Ali Saleh Aziz, 2
Riyadh Nazar Ali
1, 2
Assistant Lecturer
1, 2
Department of Medical Instruments Techniques Engineering
1, 2
Al-Hussein University College, Karbala, Iraq
________________________________________________________________________________________________________
Abstract - The aim of this paper is to design a 10W cell charger for an iPad” with restricted specifications. For this design,
the most viable and appropriate configuration of the components to fulfill the given requirements is presented. First,
parameters are calculated with hand calculation and then for analysis of the performance of the design circuit, results
from Pspice are visualized. The performance analysis which covers the non-ideal effects on related waveforms of output
voltage, current and power are discussed in details.
Index Terms - Charger, Bridge, Flyback, Ripple, Harmonic
________________________________________________________________________________________________________
I. INTRODUCTION
Nowadays, rechargeable battery has been broadly usable in various types of electronic devices, such as electrical vehicle,
uninterrupted power supply, and portable devices. Therefore, battery charger plays a vital role in recharging batteries professionally
and extending the battery life [1].
For developed countries, Power grids use AC power, whereas cell phones are charged using DC power . Therefore, AC-DC
converters are required. The chargers rectify the AC signal and convert the signal to DC for the phone battery at the specified
power rating [2].
Rectifier is a device that converts AC (Alternating Current) to DC (Direct Current). Rectifier can be classified into two groups i.e.
Half Wave and Full Wave and also each of two groups can be divided into two types of Controlled Rectifier and Uncontrolled [3].
The use of rectifiers are easily noticeable when the distribution systems are connected with nonlinear loads and the consequence of
nonlinear loads leads to harmonics which are generated in the network systems. For definition purpose, harmonics are any “Non-
Linear” Current or Voltage in an electrical distribution system which are commonly produced by devices that rectifies AC Voltage
into a DC Voltage. Harmonic frequencies in the power grid are a frequent cause of power quality problems". It is intrusive in this
paper that harmonic components should be limited in use as much as permissible [4].
Isolated converter is required in the design of a cell phone charger. Fly-back converter is the simplest type of isolated DC-DC
converters topology because there is no inductor at the output filter, only one semiconductor switch and only one magnetic
component transformer or coupled inductor. Also, fly-back converters have Low cost because of less component requirement,
Blocking voltage not occurred on the output diode, and transient response is fast because of output inductor absence . Therefore,
Fly-back converter is chosen for this study [5].
II. METHODOLOGY
Firstly the calculations have been done manually for the parameters. Then, the formulated values have been simulated using Pspice
and the results are visualized to obtain the best possible outputs.
Design Specification
The design of a 10W power adapter for the iPad has following specifications:
a) Input Supply: Single-phase 240Vrms at 50Hz.
b) Output voltage: 5.1 VDC, 5% (+ 2%) voltage ripple factor
c) Output current: 2.1A
d) The design Complies to IEC 61000-3-2 Standard: Electromagnetic Compatibility (EMC) limits for harmonic current emissions
(equipment input current ≤ 16 A per phase).
Design Calculations and Considerations
𝑉𝑜 = 𝑉𝑠 × (
𝐷
1 − 𝐷
) × (
𝑁2
𝑁1
)
Where,
D is the duty cycle.
N1 and N2 are the numbers of turns used in each of the two windings.
© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 511
𝑉𝑠(𝑝𝑒𝑎𝑘) = 𝑉𝑠(𝑟𝑚𝑠) × √2 = 240 × √2 = 339.411 𝑉
Assuming:
𝑁2
𝑁1
=
1
12
Then D=0.153
Let L1=Lmin=500 μH
Since
𝑁2
𝑁1
= √
𝐿1
𝐿2
Then: L2= 3.47 μH
The value for R3 is calculated according to the following equation:
𝑅3 =
𝑉𝑂
𝐼 𝑂
=
5.1
2.1
= 2.6 𝛺
For Sbreak : V1=0 V, V2=5V, TD =0 , TR =1ns, TF =1ns,
Where,
V1 is the initial value of the signal
V2 is the pulsed value of the signal
TD is the delay time
TR is the rise time
TF is the fall time
PW is the pulse width
PER is the period
For the simulation, the switching frequency is approximately 50 kHz
𝑃𝐸𝑅 =
1
𝑓𝑠
=
1
50 × 1000
= 20 µ 𝑠𝑒𝑐
𝑃𝑊 =
𝐷
𝑓𝑠
=
0.153
50 × 1000
= 3.06 µ 𝑠𝑒𝑐
The value of capacitor filter is calculated as follows
𝛥𝑉𝑂
𝑉𝑂
=
𝐷
𝑅3 × 𝑓𝑠 × 𝐶
→ 0.05 =
0.153
2.6 × 50 × 1000 × 𝐶
Then, C=23.5μf
Circuit Diagram of The Buck Converter
The circuit diagram of proposed design is shown in figure 1 with all parameterized variables discussed above.
© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 512
Figure 1: Simulated circuit of iPad cell charger
III. SIMULATION RESULTS AND DISCUSSION
As shown in Figure 2, the input voltage has the amplitude of 337.824V. The output voltage of rectifier, which is dc, has also been
showed.
Figure 2: Input Voltage (blue) and Output Voltage (red) of Rectifier (C1)
Figure 3 shows the input current of the circuit. It is seen that its value is nearly 10.60 A which is less than 16 A according to IEC
61000-3-2 Standard.
© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 513
Figure 3: Input Current of the Circuit
Figure 4 illustrates the Fourier series of the input current. We have brought into use the Fourier series analysis concept to match the
input current of harmonics. Figures 5, 6, 7 and 8 are showing the amplitudes of harmonics for fundamental, third, fifth and seventh
harmonics respectively. By considering the figures the corresponding harmonic amplitudes for fundamental, third, fifth and seventh
are 679.069 mA, 270.975 mA, 178.883 mA and 74.787 mA respectively. By comparing these values with table 1 which shows the
maximum permissible harmonic current for class A equipment, it is clear that the results obtained comply IEC 61000- 3-2
Standard.
Figure 4: Fourier Series of the Input Current (mA)
Figure 5: Fundamental Current (mA)
© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 514
Figure 6: Third Current Harmonic (mA)
Figure 7: Fifth Current Harmonic (mA)
Figure 8: Seventh Current Harmonic (mA)
© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 515
Table 1: Limits for Class A Equipment
But one considerable issue is that the output voltage is 𝑜 = 10.2 𝑉. This value is more than required value for output of the circuit.
the output voltage waveform is shown in figure 9.
Figure 9: Output Voltage
So for obtaining the 𝑉 𝑜 = 5.1𝑉, 𝑊2 = 𝑃𝑊/2 = 1.55µ𝑠 , 𝐷 = 0.0775 , c = 11.3μf . Figures 10, 11 and 12 show voltage, current and
power output waveforms respectively after using the new values for PW, D and C. Figure 10 shows that the output voltage of the
adapter is 5.0662 V
Figure 10: Output Voltage after using the new values for PW, D and C.
© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 516
Figure 11 illustrates that the output current of the circuit is 1.95 A. The output value for power is 10.19 W as shown in figure12.
Figure 11: Output Current after using the new values for PW, D and C.
Figure 12: Output Power after using the new values for PW, D and C.
However, we can get: 𝑉 𝑜 = 5.1𝑉 𝐼 𝑜 = 2.1𝐴 𝑃 𝑜 = 10𝑊 but the ripple is so high, so by adding a capacitor (C2 = 100μf) at the output
side we can achieve ripple = 4.7%. Figure 13 shows the simulated circuit of the cell charger with voltage ripple less than 5%.
Figure 13: Simulated circuit of cell charger with voltage ripple less than 5%.
Figure 14 shows the output voltage waveform with voltage ripple less than 5%. The output value for voltage is nearly 5.1 V which
is the desired output voltage. The percentage of ripple can be calculated by looking into the maximum and minimum output
voltages, which is shown below:
© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 517
Vo(max) = 5.3307 V and Vo(min) = 5.0910 V. Hence,
% 𝑟𝑖𝑝𝑝𝑙𝑒 =
𝑉𝑜(𝑚𝑎𝑥) − 𝑉𝑜(𝑚𝑖𝑛)
𝑉𝑜(𝑚𝑖𝑛)
× 100 =
5.3307 − 5.0910
5.0910
× 100 = 4.7%
Figure 14: Output Voltage with voltage ripple less than 5%.
According to figures 15 and 16, it is seen that the output values for current and power are approximately 2.1A and 10W
respectively
Figure 15: Output Current with for a case of voltage ripple less than 5%.
Figure 16: Output power with for a case of voltage ripple less than 5%.
© 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939
IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 518
IV. CONCLUSIONS
The optimization of the available components to its best end use efficiency has been focused on. With the same approach it was
tried to formulate and design the iPad cell charger. Combination of the components has end up in the best possible results, by
keeping in mind the specifications restrictions which have been provided. The simulation results show the steady state performance
of output voltage, current and power. The output voltage ripple can be corrected using appropriate capacitor. The results obtained
comply IEC 61000- 3-2 Standard.
REFERENCES
[1] M. M. R. Paul1, and A. Bhuvanesh, " Design and Implementation of Battery Charger Using Flyback Converter for Constant
Current and Voltage Control," International Journal for Research in Applied Science & Engineering Technology (IJRASET),
3(1): 153–159, 2015.
[2] A. Hefner and A. Magdaleno, "Cell Phone Charger for the DC House Project," B.S.c Thesis, Electrical Engineering
Department, California Polytechnic State University, 2012.
[3] M. H. Rashid, "Power Electronics: Circuits, Devices, and Applications,” 3rd Edition, Prentice Hall New Jersey, USA, 2004
[4] M. Mazaheri, V. Scaini, and W. E. Veerkamp, "Cause, Effects, and Mitigation of Ripple From Rectifiers," IEEE Trans.
Industrial Application, 39(4):1187–1192, 2003.
[5] V. L. Karthika,and N. S. George, "Design of a Power Supply Using Fly-Back Converter," International Journal of Advanced
Research in Electrical, Electronics and Instrumentation Engineering, 3(4): 403– 408, 2014.

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IJEDR1601085

  • 1. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 510 Design of a Cell Charger for an iPad Using Full Bridge Rectifier and Flyback Converter 1 Ali Saleh Aziz, 2 Riyadh Nazar Ali 1, 2 Assistant Lecturer 1, 2 Department of Medical Instruments Techniques Engineering 1, 2 Al-Hussein University College, Karbala, Iraq ________________________________________________________________________________________________________ Abstract - The aim of this paper is to design a 10W cell charger for an iPad” with restricted specifications. For this design, the most viable and appropriate configuration of the components to fulfill the given requirements is presented. First, parameters are calculated with hand calculation and then for analysis of the performance of the design circuit, results from Pspice are visualized. The performance analysis which covers the non-ideal effects on related waveforms of output voltage, current and power are discussed in details. Index Terms - Charger, Bridge, Flyback, Ripple, Harmonic ________________________________________________________________________________________________________ I. INTRODUCTION Nowadays, rechargeable battery has been broadly usable in various types of electronic devices, such as electrical vehicle, uninterrupted power supply, and portable devices. Therefore, battery charger plays a vital role in recharging batteries professionally and extending the battery life [1]. For developed countries, Power grids use AC power, whereas cell phones are charged using DC power . Therefore, AC-DC converters are required. The chargers rectify the AC signal and convert the signal to DC for the phone battery at the specified power rating [2]. Rectifier is a device that converts AC (Alternating Current) to DC (Direct Current). Rectifier can be classified into two groups i.e. Half Wave and Full Wave and also each of two groups can be divided into two types of Controlled Rectifier and Uncontrolled [3]. The use of rectifiers are easily noticeable when the distribution systems are connected with nonlinear loads and the consequence of nonlinear loads leads to harmonics which are generated in the network systems. For definition purpose, harmonics are any “Non- Linear” Current or Voltage in an electrical distribution system which are commonly produced by devices that rectifies AC Voltage into a DC Voltage. Harmonic frequencies in the power grid are a frequent cause of power quality problems". It is intrusive in this paper that harmonic components should be limited in use as much as permissible [4]. Isolated converter is required in the design of a cell phone charger. Fly-back converter is the simplest type of isolated DC-DC converters topology because there is no inductor at the output filter, only one semiconductor switch and only one magnetic component transformer or coupled inductor. Also, fly-back converters have Low cost because of less component requirement, Blocking voltage not occurred on the output diode, and transient response is fast because of output inductor absence . Therefore, Fly-back converter is chosen for this study [5]. II. METHODOLOGY Firstly the calculations have been done manually for the parameters. Then, the formulated values have been simulated using Pspice and the results are visualized to obtain the best possible outputs. Design Specification The design of a 10W power adapter for the iPad has following specifications: a) Input Supply: Single-phase 240Vrms at 50Hz. b) Output voltage: 5.1 VDC, 5% (+ 2%) voltage ripple factor c) Output current: 2.1A d) The design Complies to IEC 61000-3-2 Standard: Electromagnetic Compatibility (EMC) limits for harmonic current emissions (equipment input current ≤ 16 A per phase). Design Calculations and Considerations 𝑉𝑜 = 𝑉𝑠 × ( 𝐷 1 − 𝐷 ) × ( 𝑁2 𝑁1 ) Where, D is the duty cycle. N1 and N2 are the numbers of turns used in each of the two windings.
  • 2. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 511 𝑉𝑠(𝑝𝑒𝑎𝑘) = 𝑉𝑠(𝑟𝑚𝑠) × √2 = 240 × √2 = 339.411 𝑉 Assuming: 𝑁2 𝑁1 = 1 12 Then D=0.153 Let L1=Lmin=500 μH Since 𝑁2 𝑁1 = √ 𝐿1 𝐿2 Then: L2= 3.47 μH The value for R3 is calculated according to the following equation: 𝑅3 = 𝑉𝑂 𝐼 𝑂 = 5.1 2.1 = 2.6 𝛺 For Sbreak : V1=0 V, V2=5V, TD =0 , TR =1ns, TF =1ns, Where, V1 is the initial value of the signal V2 is the pulsed value of the signal TD is the delay time TR is the rise time TF is the fall time PW is the pulse width PER is the period For the simulation, the switching frequency is approximately 50 kHz 𝑃𝐸𝑅 = 1 𝑓𝑠 = 1 50 × 1000 = 20 µ 𝑠𝑒𝑐 𝑃𝑊 = 𝐷 𝑓𝑠 = 0.153 50 × 1000 = 3.06 µ 𝑠𝑒𝑐 The value of capacitor filter is calculated as follows 𝛥𝑉𝑂 𝑉𝑂 = 𝐷 𝑅3 × 𝑓𝑠 × 𝐶 → 0.05 = 0.153 2.6 × 50 × 1000 × 𝐶 Then, C=23.5μf Circuit Diagram of The Buck Converter The circuit diagram of proposed design is shown in figure 1 with all parameterized variables discussed above.
  • 3. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 512 Figure 1: Simulated circuit of iPad cell charger III. SIMULATION RESULTS AND DISCUSSION As shown in Figure 2, the input voltage has the amplitude of 337.824V. The output voltage of rectifier, which is dc, has also been showed. Figure 2: Input Voltage (blue) and Output Voltage (red) of Rectifier (C1) Figure 3 shows the input current of the circuit. It is seen that its value is nearly 10.60 A which is less than 16 A according to IEC 61000-3-2 Standard.
  • 4. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 513 Figure 3: Input Current of the Circuit Figure 4 illustrates the Fourier series of the input current. We have brought into use the Fourier series analysis concept to match the input current of harmonics. Figures 5, 6, 7 and 8 are showing the amplitudes of harmonics for fundamental, third, fifth and seventh harmonics respectively. By considering the figures the corresponding harmonic amplitudes for fundamental, third, fifth and seventh are 679.069 mA, 270.975 mA, 178.883 mA and 74.787 mA respectively. By comparing these values with table 1 which shows the maximum permissible harmonic current for class A equipment, it is clear that the results obtained comply IEC 61000- 3-2 Standard. Figure 4: Fourier Series of the Input Current (mA) Figure 5: Fundamental Current (mA)
  • 5. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 514 Figure 6: Third Current Harmonic (mA) Figure 7: Fifth Current Harmonic (mA) Figure 8: Seventh Current Harmonic (mA)
  • 6. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 515 Table 1: Limits for Class A Equipment But one considerable issue is that the output voltage is 𝑜 = 10.2 𝑉. This value is more than required value for output of the circuit. the output voltage waveform is shown in figure 9. Figure 9: Output Voltage So for obtaining the 𝑉 𝑜 = 5.1𝑉, 𝑊2 = 𝑃𝑊/2 = 1.55µ𝑠 , 𝐷 = 0.0775 , c = 11.3μf . Figures 10, 11 and 12 show voltage, current and power output waveforms respectively after using the new values for PW, D and C. Figure 10 shows that the output voltage of the adapter is 5.0662 V Figure 10: Output Voltage after using the new values for PW, D and C.
  • 7. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 516 Figure 11 illustrates that the output current of the circuit is 1.95 A. The output value for power is 10.19 W as shown in figure12. Figure 11: Output Current after using the new values for PW, D and C. Figure 12: Output Power after using the new values for PW, D and C. However, we can get: 𝑉 𝑜 = 5.1𝑉 𝐼 𝑜 = 2.1𝐴 𝑃 𝑜 = 10𝑊 but the ripple is so high, so by adding a capacitor (C2 = 100μf) at the output side we can achieve ripple = 4.7%. Figure 13 shows the simulated circuit of the cell charger with voltage ripple less than 5%. Figure 13: Simulated circuit of cell charger with voltage ripple less than 5%. Figure 14 shows the output voltage waveform with voltage ripple less than 5%. The output value for voltage is nearly 5.1 V which is the desired output voltage. The percentage of ripple can be calculated by looking into the maximum and minimum output voltages, which is shown below:
  • 8. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 517 Vo(max) = 5.3307 V and Vo(min) = 5.0910 V. Hence, % 𝑟𝑖𝑝𝑝𝑙𝑒 = 𝑉𝑜(𝑚𝑎𝑥) − 𝑉𝑜(𝑚𝑖𝑛) 𝑉𝑜(𝑚𝑖𝑛) × 100 = 5.3307 − 5.0910 5.0910 × 100 = 4.7% Figure 14: Output Voltage with voltage ripple less than 5%. According to figures 15 and 16, it is seen that the output values for current and power are approximately 2.1A and 10W respectively Figure 15: Output Current with for a case of voltage ripple less than 5%. Figure 16: Output power with for a case of voltage ripple less than 5%.
  • 9. © 2016 IJEDR | Volume 4, Issue 1 | ISSN: 2321-9939 IJEDR1601085 International Journal of Engineering Development and Research (www.ijedr.org) 518 IV. CONCLUSIONS The optimization of the available components to its best end use efficiency has been focused on. With the same approach it was tried to formulate and design the iPad cell charger. Combination of the components has end up in the best possible results, by keeping in mind the specifications restrictions which have been provided. The simulation results show the steady state performance of output voltage, current and power. The output voltage ripple can be corrected using appropriate capacitor. The results obtained comply IEC 61000- 3-2 Standard. REFERENCES [1] M. M. R. Paul1, and A. Bhuvanesh, " Design and Implementation of Battery Charger Using Flyback Converter for Constant Current and Voltage Control," International Journal for Research in Applied Science & Engineering Technology (IJRASET), 3(1): 153–159, 2015. [2] A. Hefner and A. Magdaleno, "Cell Phone Charger for the DC House Project," B.S.c Thesis, Electrical Engineering Department, California Polytechnic State University, 2012. [3] M. H. Rashid, "Power Electronics: Circuits, Devices, and Applications,” 3rd Edition, Prentice Hall New Jersey, USA, 2004 [4] M. Mazaheri, V. Scaini, and W. E. Veerkamp, "Cause, Effects, and Mitigation of Ripple From Rectifiers," IEEE Trans. Industrial Application, 39(4):1187–1192, 2003. [5] V. L. Karthika,and N. S. George, "Design of a Power Supply Using Fly-Back Converter," International Journal of Advanced Research in Electrical, Electronics and Instrumentation Engineering, 3(4): 403– 408, 2014.