The Single-Phase-Shift (SPS)
modulation is the most fundamental and widely adopted control method for the Dual
Active Bridge (DAB) converter. Under SPS control, both the primary-side full bridge
(Bridge 1) and the secondary-side full bridge (Bridge 2) operate at a fixed 50% duty
cycle. The diagonal switch pairs of each bridge (such as Q1/Q4 and Q5/Q8) are turned
on and off synchronously .
The core control variable in this scheme is the
external phase-shift angle
introduced between the primary-side square-wave
voltage (Vp) and the secondary-side square-wave voltage
(Vs). This phase shift angle directly regulates the direction
and magnitude of the power flow across the high-frequency isolation transformer T1,
as shown in Figure 2-4.
The average power P12 transferred between the two bridges is
governed by the energy stored and released in the series leakage inductor
Ls, which can be mathematically expressed as
:
Equation 1.
Where V1 is the input DC voltage,
V2 is the output DC voltage, fs is the
switching frequency, and N is the transformer turns ratio (N =
N1/N2) .
- Forward Power Mode (
): Vp leads
Vs, causing energy to flow from the primary side to the
secondary side .
- Reverse Power Mode (
): Vp lags
Vs, causing energy to seamlessly flow back from the
secondary side to the primary side.
The maximum power capability (
Pmax) is strictly limited by the
hardware parameters
Ls and
fs, and is achieved when
the phase-shift angle
equals
:
Equation 2.
To minimize switching losses and achieve high total system efficiency, the
SPS-DAB relies entirely on the reactive energy stored in the leakage inductor
Ls to discharge and charge the MOSFET parasitic output
capacitances Coss, thereby facilitating Zero Voltage Switching
(ZVS). Figure 2-5
shows complete waveforms of PWM and current . Taking the forward operation mode as a
reference, a typical switching cycle progresses through the following key
intervals:
- Interval 1 (
to
- Dead Time Realization, as shown in
Figure 2-6): Prior to
, the switches Q1 and Q4 are turned off .
During this dead-time interval, the inductor current IL must
remain negative (
). This negative current forces the energy stored
in Ls to discharge the output capacitances of Q1 and Q4 while
charging those of Q2 and Q3, creating the necessary zero-voltage condition
across Q1 and Q4 prior to their turn-on .
- Interval 2 (
to
- Primary Channel Conduction, as shown in
Figure 2-7): At
, switches Q1 and Q4 are turned on under
a strict zero-voltage condition(Ideal situation). The inductor current passes
through the channels of Q1 and Q4, and begins to rise linearly .
- Interval 3 (
to
- Current Reversal, as shown in Figure
2-8): At
, the inductor current crosses zero and
switches its direction to positive, continuing its linear progression driven by
the voltage difference across the transformer.
- Interval 4 (
to
- Secondary Side ZVS Realization, as
shown in Figure 2-9): At
, the secondary side switches Q5 and Q8
are turned off . To enable ZVS for the secondary bridge, the inductor current at
this moment must be positive (
). This positive transformer current successfully
discharges the output capacitances of Q5 and Q8 while charging Q6 and Q7 during
the secondary side dead time.
- Interval 5 (
to
) - Full Commutation, as shown in Figure
2-9): At
, Q5 and Q8 achieve soft turn-on. The
current flows naturally through the secondary bridge channels, completing the
primary-to-secondary power commutation phase until the next half-cycle repeats
the identical process for the remaining FETs from
to
.