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22-Elec-B8 Power Electronics and Drives · May 2018

Question 4 of 6: Problem 3 — basic dc chopper with an R–L load

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams, May 2018 — 16-Elec-B8, Power Electronics and Drives. Open book, three hours, any non-communicating calculator permitted. The paper is in two parts: Part 1 is twenty short-answer items (a) to (t) worth 2.5 points each, and Part 2 is five calculation problems worth 15 points each. The rubric says “attempt all parts” and that the maximum total score of 125 points includes a bonus of 25 points, so a candidate scoring 100 of the 125 available marks has a full paper. Every item and every sub-part is worked below.

Reference texts.

Question 4: Problem 3 — basic dc chopper with an R–L load (15 points)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. A step-down chopper switches a 24 V source into a series R–L load at a fixed 2 ms period, and the duty ratio is specified indirectly through the ripple, as the ratio of minimum to maximum load current.

Given data
QuantitySymbolValue
Input voltage$V_{i}$24 V
Chopping period$T$2 ms
Load resistance$R$1.8 Ω
Load inductance$L$0.45 mH
Current ratio$I_{min}/I_{max}$0.75
Sample instants$t$1 ms and 1.5 ms

Find. (a) the load time constant and the on-time; (b) the peak and valley load currents; (c) the time-domain current expressions for both sub-intervals and the current at $t=1$ ms and $t=1.5$ ms.

Problem 3: chopper load current over one periodload current i(t), vertical axis brokenImax = 13.332 AImin = 9.999 Aturn-off at t = 1.9281 mst = 1.00 ms: i = 13.272 At = 1.50 ms: i = 13.325 A0.00 ms0.50 ms1.00 ms1.50 ms2.00 ms
The load time constant is only an eighth of the period, so the current is fully settled for most of the on-time and the whole ripple is squeezed into the last 3.6 per cent of the period. Both sample instants therefore fall in the on-interval. Note the broken vertical axis.

Approach. During the free-wheel interval no source is present, so the current is a pure decaying exponential and the stated current ratio fixes the off-time on its own; only then do the steady-state boundary conditions fix the current levels.

  1. Compute the load time constant. $$\tau=\frac{L}{R}=\frac{0.45\times10^{-3}}{1.8}=\boxed{0.250\ \text{ms}}$$
  2. Extract the off-time from the ratio alone. With the switch open the load free-wheels through the diode with no driving source, so $i(t)=I_{max}e^{-t/\tau}$ and $$\frac{I_{min}}{I_{max}}=e^{-t_{off}/\tau}\ \Rightarrow\ t_{off}=-\tau\ln(0.75)=0.250\times0.28768=0.0719\ \text{ms}$$ The current magnitudes never enter this step.
  3. Hence the on-time and the duty ratio. $$t_{on}=T-t_{off}=2.000-0.0719=\boxed{1.9281\ \text{ms}}\qquad \delta=\frac{t_{on}}{T}=0.9640$$

With the levels still unknown, the periodic steady state supplies them. Matching the end of the rising interval to the start of the decaying one and requiring the waveform to repeat gives the standard pair of boundary conditions.

  1. Solve the steady-state peak. $$I_{max}=\frac{V_{i}}{R}\cdot\frac{1-e^{-t_{on}/\tau}}{1-e^{-T/\tau}}=13.333\times\frac{1-e^{-7.7123}}{1-e^{-8}}=\boxed{13.332\ \text{A}}$$
  2. And the valley from the given ratio. $$I_{min}=0.75\,I_{max}=0.75\times13.3318=\boxed{9.999\ \text{A}}$$ The peak-to-peak ripple is therefore 3.333 A.

Two checks close part (b). The mean current predicted by the duty ratio, $\delta V_{i}/R=0.9640\times24/1.8=12.85$ A, lies between the valley and the peak as it must. And the widely used linear-ripple estimate $\Delta I\approx V_{i}\delta(1-\delta)T/L$ returns 3.698 A against the true 3.333 A, an 11 per cent error, because that shortcut assumes $\tau\gg T$ whereas here $\tau$ is an eighth of $T$. The exponential forms must be used.

  1. Write the on-interval expression. Measuring $t$ from the switch turning on, with initial value $I_{min}$: $$i_{on}(t)=\frac{V_{i}}{R}\left(1-e^{-t/\tau}\right)+I_{min}e^{-t/\tau}=13.332-3.333\,e^{-t/0.25\ \text{ms}}$$ valid for $0\le t\le 1.9281$ ms.
  2. Write the off-interval expression. Measuring $t^{\prime}$ from turn-off, $$i_{off}(t^{\prime})=I_{max}e^{-t^{\prime}/\tau}=13.332\,e^{-t^{\prime}/0.25\ \text{ms}}$$ valid for $0\le t^{\prime}\le0.0719$ ms.
  3. Screen each requested instant against the on-time before choosing a branch. Both 1 ms and 1.5 ms are less than $t_{on}=1.9281$ ms, so both lie in the on-interval and $i_{on}$ applies to each.
  4. Evaluate. $e^{-4}=0.018316$ and $e^{-6}=0.0024788$, so $$i(1\ \text{ms})=13.332-3.333\times0.018316=\boxed{13.272\ \text{A}}$$ $$i(1.5\ \text{ms})=13.332-3.333\times0.0024788=\boxed{13.325\ \text{A}}$$

Both values sit within half a per cent of $V_{i}/R=13.333$ A. That flatness is the correct answer, not a slip: four time constants have already elapsed by 1 ms, so the current has settled to its resistive limit long before the switch opens.

Final results
QuantitySymbolResult
Load time constant$\tau=L/R$0.250 ms
Off-time$t_{off}$0.0719 ms
On-time$t_{on}$1.9281 ms
Duty ratio$\delta$0.9640
Maximum load current$I_{max}$13.332 A
Minimum load current$I_{min}$9.999 A
Peak-to-peak ripple$\Delta I$3.333 A
Current at $t=1$ ms$i(1\ \text{ms})$13.272 A
Current at $t=1.5$ ms$i(1.5\ \text{ms})$13.325 A
Check: the drive is being run at the edge of its useful design space. A 25 per cent ripple ratio at $\tau/T=0.125$ forces a duty of 0.964, so the entire free-wheel interval is 72 µs long — less than a third of one time constant, and short enough that switch turn-off and diode recovery times become a real fraction of it. The engineering fix for a ripple specification this tight is a higher switching frequency (a shorter $T$ raises $I_{min}/I_{max}$ at any duty), not a higher duty ratio. The numbers above answer the question as set; the design comment belongs with them.