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DC Power Supplies slides

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DC Power Supplies
S.S. Abeywickrama
DC power supplies
Why DC power sources ?
Most electronic devices and circuits require a DC source for their operations.
What can perform as a DC Source ?
1. Electrical cells
2. Batteries
3. conventional DC power supplies
Why DC Power supplies?
οƒΌMost Convenient
οƒΌEconomical
οƒΌNo replacements
DC power supply
AC
Mains
Step -Down
Transformer
Rectifier
V
Voltage
regulator
Filter
V
V
V
V
t
t
LOAD
t
t
V
t
Block Diagram of the Dc power supply
t
Step-down Transformer
Step-down transformer is used to reduce the amplitude of the AC voltage
and it provides following advantages
• works as an isolator between AC source and rectifier circuit
• Reduces the chance of getting electric shocks
Where:
VP - is the Primary Voltage
VS - is the Secondary Voltage
NP - is the Number of Primary Windings
NS - is the Number of Secondary Windings
Step-Down Transformer
Center-tapped Transformer
This type of transformers are used to construct two output signals with
same amplitude and 1800 phase difference
Rectifier
A Rectifier is a circuit that can convert the AC signals into pulsating DC
Signals. Two types of rectifiers are available
1. Half-wave rectifier
2. Full-wave rectifier
pulsating DC Signals
Half-wave rectifier
Half-wave rectifier circuit
Transformer:
VS –instantaneous voltage of the secondary winding
VS(max) –peak voltage of the secondary winding
Load:
VL –instantaneous voltage of the load resistor
IL –instantaneous current of the load resistor
IL(max) –maximum value of the load current
VL(max) –maximum value of the voltage across the load resistor
VL (rms) – rms value of the entire voltage across the load resistor
VL
VL
(DC)
(AC)
–DC value of the voltage across the load resistor
–rms value of the AC components of the voltage across the load resistor
Half-wave rectifier circuit
Ripple factor
Ripple factor,  =
π‘Ÿπ‘šπ‘  π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ 𝐴𝐢 π‘π‘œπ‘šπ‘π‘œπ‘›π‘’π‘›π‘‘π‘  π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘ π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’
𝐷𝐢 π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘ π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’
VL (AC)
=
VL (DC)
for a half-wave rectifier,  =1.21
Efficiency
Efficiency ,  =
𝐷𝐢 π‘π‘œπ‘€π‘’π‘Ÿ π‘‘π‘’π‘™π‘–π‘£π‘’π‘Ÿπ‘’π‘‘ π‘‘π‘œ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘
π‘‡π‘œπ‘‘π‘Žπ‘™ π‘π‘œπ‘€π‘’π‘Ÿ π‘‘π‘–π‘ π‘ π‘Žπ‘π‘Žπ‘‘π‘–π‘œπ‘›
IL (DC)2RL
=
× 100%
2
IL (rms) (RL+RD+Rs)
PL (DC)
× 100% =
× 100%
PL (Total)
Half-wave rectifier circuit
Peak inverse voltage (PIV):
It is the maximum voltage occurs across the rectifying diode in the reverse
direction.
For a half-wave rectifier, diode is reverse biased during the negative half-cycle
PIV equals the maximum voltage across the secondary voltage.
Full-wave rectifier with center-tapped transformer
Full-wave rectifier with center-tapped transformer
Transformer:
VS –instantaneous voltage of the secondary winding
VS(max) –peak voltage of the secondary winding
Load:
VL –instantaneous voltage of the load resistor
IL –instantaneous current of the load resistor
IL(max) –maximum value of the load current
VL(max) –maximum value of the voltage across the load resistor
VL (rms) – rms value of the entire voltage across the load resistor
VL (DC) –DC value of the voltage across the load resistor
VL (AC) –rms value of the AC components of the voltage across the load resistor
Full-wave rectifier with center-tapped transformer
Ripple factor
Ripple factor,  =
π‘Ÿπ‘šπ‘  π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ 𝐴𝐢 π‘π‘œπ‘šπ‘π‘œπ‘›π‘’π‘›π‘‘π‘  π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘ π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’
𝐷𝐢 π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘ π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’
VL (AC)
=
VL (DC)
for a half-wave rectifier,  =0.482
Efficiency
Efficiency ,  =
𝐷𝐢 π‘π‘œπ‘€π‘’π‘Ÿ π‘‘π‘’π‘™π‘–π‘£π‘’π‘Ÿπ‘’π‘‘ π‘‘π‘œ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘
π‘‡π‘œπ‘‘π‘Žπ‘™ π‘π‘œπ‘€π‘’π‘Ÿ π‘‘π‘–π‘ π‘ π‘Žπ‘π‘Žπ‘‘π‘–π‘œπ‘›
PL (DC)
× 100% =
× 100%
PL (Total)
IL (DC)2RL
=
× 100%
2
IL (rms) (RL+rD+Rs)
Here, Rs is considered as resistance of one secondary winding.
Full-wave rectifier with center-tapped transformer
Peak inverse voltage (PIV):
For a full-wave rectifier with center-tapped transformer,
PIV = 2VS(max)
(VS(max) is the maximum voltage across one of its secondary windings)
Full-wave bridge rectifier
Full-wave bridge rectifier
full-wave bridge rectifier
Transformer:
VS –instantaneous voltage of the secondary winding
VS(max) –peak voltage of the secondary winding
Load:
VL –instantaneous voltage of the load resistor
IL –instantaneous current of the load resistor
IL(max) –maximum value of the load current
VL(max) –maximum value of the voltage across the load resistor
VL (rms) – rms value of the entire voltage across the load resistor
VL
VL
(DC)
(AC)
–DC value of the voltage across the load resistor
–rms value of the AC components of the voltage across the load resistor
full-wave bridge rectifier
Ripple factor
Ripple factor,  =
π‘Ÿπ‘šπ‘  π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ 𝐴𝐢 π‘π‘œπ‘šπ‘π‘œπ‘›π‘’π‘›π‘‘π‘  π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘ π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’
𝐷𝐢 π‘£π‘Žπ‘™π‘’π‘’ π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘ π‘£π‘œπ‘™π‘‘π‘Žπ‘”π‘’
VL (AC)
=
VL (DC)
for a half-wave rectifier,  =0.482
Efficiency
Efficiency ,  =
𝐷𝐢 π‘π‘œπ‘€π‘’π‘Ÿ π‘‘π‘’π‘™π‘–π‘£π‘’π‘Ÿπ‘’π‘‘ π‘‘π‘œ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘
π‘‡π‘œπ‘‘π‘Žπ‘™ π‘π‘œπ‘€π‘’π‘Ÿ π‘‘π‘–π‘ π‘ π‘Žπ‘π‘Žπ‘‘π‘–π‘œπ‘› π‘œπ‘“ π‘‘β„Žπ‘’ π‘™π‘œπ‘Žπ‘‘
IL (DC)2RL
=
× 100%
2
IL (rms) (RL+2rD+Rs)
PL (DC)
× 100% =
× 100%
PL (Total)
Full-wave bridge rectifier
Peak inverse voltage (PIV):
For a full-wave rectifier with center-tapped transformer,
PIV = VS(max)
(VS(max) is the maximum voltage across the secondary winding)
Filter
Output of various rectifier circuits has pulsating. It has a DC and some AC
components called as ripple. This kind of pulsating output is not useful for
driving a sophisticated electronic device or circuit. The main function of filter is
the minimization of ripple content in the rectifier output.
Type of Filters
• Shunt capacitor filter
• Series inductor filter
• L-C Filter
• R-C Filter
Shunt capacitor filter
Shunt capacitor filter is made by connecting a capacitor across the load
resistor.
Shunt capacitor filter
Shunt capacitor filter reduces the Ripple factor, and increases the DC
value of the output voltage.
For a Half-wave rectifier
1
=
2 3𝑓𝐢𝑅
𝑉𝐷𝐢 =
2𝑓𝐢𝑅
𝑉
1 + 2𝑓𝐢𝑅 𝑝
For a full-wave rectifier
1
=
4 3𝑓𝐢𝑅
𝑉𝐷𝐢 =
Where; C- Capacitance of the capacitor in the filter
R- resistance of the Load resistor
f- Frequency of the transformer
𝑉𝑝 - peak/maximum value of the rectifier’s output voltage
4𝑓𝐢𝑅
𝑉
1 + 4𝑓𝐢𝑅 𝑝
Voltage Regulator
• Voltage regulator can be considered as the final stage of a DC power
supply.
• Power supply without a voltage regulator is known as an unregulated power
supply.
• An unregulated power supply can not be used to supply a constant voltage
across a load.
RS
RL
variable load
VS
Variable Voltage Source
Unregulated Power Supply
Voltage Regulator
Voltage Regulator is a electronic circuit which maintains a
constant voltage across the load in spite of the input voltage
variations (line fluctuations) or load variations (Load fluctuations).
The ability of a power supply to maintain a constant output voltage under the
line or load fluctuations is known as the voltage regulation. Mathematically the
voltage regulation is given by,
Voltage regulation =
𝑉𝑁𝐿 − 𝑉𝐹𝐿
𝑉𝐹𝐿
where; 𝑉𝐹𝐿 is the open-circuit voltage and 𝑉𝑁𝐿 is full-load voltage of the power
supply.
Types of Voltage Regulators
• Zener diode shunt voltage regulator
• Transistor shunt voltage regulator
• Transistor series voltage regulator
• Monolithic voltage regulator
Zener diode shunt voltage regulator
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