2.3.2Diodes & Applications

Full-wave and bridge rectifiers

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WHAT is a full-wave rectifier?

WHY two topologies? Both achieve the same goal (flip the negative half up). They differ in how they route the current so that current always flows the same direction through the load.


HOW the center-tapped rectifier works

Picture a transformer secondary split at the middle into a top half and a bottom half, sharing a common center point (the tap = 0 V reference).

  • On the positive half-cycle: the top winding is positive, so diode D1D_1 conducts, current flows through RLR_L top→bottom.
  • On the negative half-cycle: the bottom winding is positive, so diode D2D_2 conducts, current flows through RLR_L in the same direction.

Only one diode conducts at a time, so you lose one diode drop (0.70.7 V for silicon).

Vout,peak=Vsecondary,peak20.7 VV_{out,peak} = \frac{V_{secondary,peak}}{2} - 0.7\text{ V}

(the "/2" because each half of the secondary only carries half the total secondary voltage.)


HOW the bridge rectifier works

Four diodes arranged in a diamond. AC comes in on two corners; the load sits across the other two.

  • On the positive half-cycle: diodes D1D_1 and D2D_2 (a diagonal pair) conduct.
  • On the negative half-cycle: the other diagonal pair D3D_3 and D4D_4 conduct.

In both cases current is steered through RLR_L in the same direction.

Two diodes conduct in series each half-cycle, so you lose two diode drops:

Vout,peak=Vsecondary,peak2(0.7 V)V_{out,peak} = V_{secondary,peak} - 2(0.7\text{ V})

Figure — Full-wave and bridge rectifiers

DERIVATION: Average (DC) value from first principles

We want the average height of the rectified waveform. The full-wave output is v(t)=Vmsinωtv(t)=V_m|\sin\omega t|.

Average over one full period T=2πωT=\frac{2\pi}{\omega}. Because the two humps are identical, average over just half a period [0,π/ω][0,\pi/\omega]:

Vdc=1π/ω0π/ωVmsin(ωt)dtV_{dc}=\frac{1}{\pi/\omega}\int_0^{\pi/\omega} V_m\sin(\omega t)\,dt

Let θ=ωt\theta=\omega t, dθ=ωdtd\theta=\omega\,dt:

Vdc=Vmπ0πsinθdθ=Vmπ[cosθ]0π=Vmπ[(1)(1)]V_{dc}=\frac{V_m}{\pi}\int_0^{\pi}\sin\theta\,d\theta=\frac{V_m}{\pi}\big[-\cos\theta\big]_0^{\pi}=\frac{V_m}{\pi}\big[-(-1)-(-1)\big]

Vdc=2Vmπ0.637Vm\boxed{V_{dc}=\frac{2V_m}{\pi}\approx 0.637\,V_m}

Why this step? The integral is the "total area" under one hump; dividing by the width gives the average height — that is literally what a DC meter reads.

Compare: half-wave gives Vdc=Vm/π0.318VmV_{dc}=V_m/\pi\approx0.318V_m. Full-wave is exactly double — makes sense, we kept both humps.


DERIVATION: RMS value

Vrms=1π0π(Vmsinθ)2dθ=Vm1π0πsin2θdθV_{rms}=\sqrt{\frac{1}{\pi}\int_0^{\pi}(V_m\sin\theta)^2\,d\theta}=V_m\sqrt{\frac{1}{\pi}\int_0^{\pi}\sin^2\theta\,d\theta}

Use sin2θ=12(1cos2θ)\sin^2\theta=\tfrac{1}{2}(1-\cos2\theta):

0πsin2θdθ=12[θsin2θ2]0π=π2\int_0^\pi\sin^2\theta\,d\theta=\frac{1}{2}\Big[\theta-\frac{\sin2\theta}{2}\Big]_0^\pi=\frac{\pi}{2}

Vrms=Vm20.707Vm\boxed{V_{rms}=\frac{V_m}{\sqrt2}\approx0.707\,V_m}

Why this matters: rectifying doesn't change RMS vs. the full sine, because squaring erases the sign difference.


DERIVATION: Ripple factor & efficiency

Why derive rr this way? Any waveform = DC part + AC (ripple) part. Vrms2=Vdc2+Vac,rms2V_{rms}^2 = V_{dc}^2 + V_{ac,rms}^2 (they're orthogonal). Rearranging gives Vac,rms=Vrms2Vdc2V_{ac,rms}=\sqrt{V_{rms}^2-V_{dc}^2}, then divide by VdcV_{dc}.

Ripple frequency =2f=2f (two humps per input cycle) — key advantage: a smoothing capacitor of the same size filters full-wave ripple far better than half-wave.

Rectification efficiency: η=PdcPac=(2Vm/π)2(Vm/2)2=4/π21/2=8π281.2%\eta=\dfrac{P_{dc}}{P_{ac}}=\dfrac{(2V_m/\pi)^2}{(V_m/\sqrt2)^2}=\dfrac{4/\pi^2}{1/2}=\dfrac{8}{\pi^2}\approx81.2\% (double the half-wave's 40.6%).


Worked Examples



Active Recall

Recall Cover and answer
  1. Why is full-wave VdcV_{dc} exactly double the half-wave value?
  2. How many diodes conduct at once in a bridge? In a center-tapped?
  3. Which topology needs the higher PIV diodes, and by what factor?
  4. What is the ripple frequency for a 60 Hz supply?
  5. Derive Vdc=2Vm/πV_{dc}=2V_m/\pi in two lines.
Recall Explain to a 12-year-old (Feynman)

Imagine a swing that goes forward and backward. A half-wave rectifier only lets you push it when it swings forward — half the pushes are wasted. A full-wave rectifier is a smart friend who catches the swing on the backswing too and turns that into a forward push. So the swing gets pushed twice as often and moves much more smoothly. The "bridge" version does this with four one-way gates so the swing always ends up going the same way, no matter which direction it started.


Flashcards

What is VdcV_{dc} of a full-wave rectifier in terms of VmV_m?
Vdc=2Vmπ0.637VmV_{dc}=\dfrac{2V_m}{\pi}\approx0.637V_m
What is VrmsV_{rms} of a full-wave rectified sine?
Vm20.707Vm\dfrac{V_m}{\sqrt2}\approx0.707V_m
Ripple factor of a full-wave rectifier?
r0.48r\approx0.48
Ripple frequency vs. input frequency ff?
2f2f (two humps per cycle)
How many diodes conduct simultaneously in a bridge rectifier?
Two (a diagonal pair) in series
How many diodes conduct at a time in a center-tapped rectifier?
One
PIV of each diode in a center-tapped rectifier?
2Vm\approx 2V_m
PIV of each diode in a bridge rectifier?
Vm\approx V_m
Output peak of a bridge rectifier (Si)?
Vm2(0.7)V_m - 2(0.7) V
Output peak of a center-tapped rectifier (Si)?
Vsec,peak20.7\dfrac{V_{sec,peak}}{2} - 0.7 V
Rectification efficiency of a full-wave rectifier?
8/π281.2%8/\pi^2\approx81.2\%
Why does bridge use less transformer copper than center-tap?
It needs no center tap and uses the full secondary each half-cycle

Connections

  • Half-wave rectifiers — the 50%-wasteful predecessor
  • Capacitor filter / smoothing — exploits the 2f2f ripple for smaller caps
  • Peak Inverse Voltage (PIV) — selects diode ratings
  • Diode I-V characteristics — origin of the 0.70.7 V drop
  • Transformers — center-tap vs. full secondary
  • Zener regulator — what comes after smoothing
  • RMS and average values — the integral machinery reused here

Concept Map

both halves flipped up

output pulses

topology 1

topology 2

requires

one diode conducts

no center tap, diamond of 4

gives

gives

current same direction through

integrate abs sine

AC input sine wave

Full-wave rectifier

Twice ripple frequency

Center-tapped two-diode

Bridge four-diode

Transformer center tap

Loses one 0.7V drop

Loses two 0.7V drops

Vout = Vsec/2 - 0.7V

Vout = Vsec - 1.4V

Load RL

Average DC value Vdc

Hinglish (regional understanding)

Intuition Hinglish mein samjho

Dekho, half-wave rectifier AC ka sirf ek half (positive) leta hai aur negative half ko phenk deta hai — matlab aadhi power waste. Full-wave rectifier smart hai: wo negative half ko delete karne ke bajaye usse ulta karke upar flip kar deta hai. Isse output mein ek cycle mein do humps aate hain, isliye ripple frequency 2f2f ho jaati hai aur DC zyada smooth milta hai. Yehi reason hai ki phir chhota capacitor bhi easily filter kar deta hai.

Do designs hote hain. Center-tapped mein transformer ke beech mein ek tap hota hai; jo half positive ho jaaye, uska diode current ko load ke through same direction mein bhej deta hai. Yahan ek time par sirf ek diode conduct karta hai, isliye sirf 0.70.7 V drop, lekin har diode ko 2Vm2V_m ka PIV jhelna padta hai. Bridge design mein 4 diodes ek diamond shape mein lage hote hain; do-do diode ka diagonal pair alternate half-cycles mein on hota hai. Yahan do diode series mein conduct karte hain (1.41.4 V drop) par PIV sirf VmV_m — isliye high voltage supplies mein bridge sasta padta hai.

Important formulas yaad rakho: Vdc=2Vm/π0.637VmV_{dc}=2V_m/\pi\approx0.637V_m (half-wave ka bilkul double), Vrms=Vm/20.707VmV_{rms}=V_m/\sqrt2\approx0.707V_m, aur ripple factor 0.48\approx0.48 (half-wave ka 1.211.21 se kaafi kam). Efficiency 8/π281%8/\pi^2\approx81\%. Exam mein trap yeh hota hai ki log same output voltage maan lete hain dono designs ka — nahi! Pehle effective VmV_m nikaalo, phir sahi number of diode drops subtract karo (center-tap = 1, bridge = 2). Bas yeh dhyan rakhoge to sab sawaal ho jaayenge.

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