CCommons

Choke coil reduces AC current without wasting power, but a resistor does. Where does the energy go?

Pooja Iyer12th Sample

4 Sept 2026 · 1 min read

NCERT says a choke coil is used to reduce current in an AC circuit with almost no power loss, while a resistor would waste it as heat. I do NOT get this. Current drops in both cases!

For a series L–R circuit, Irms=VrmsR2+XL2I_{rms} = \dfrac{V_{rms}}{\sqrt{R^2 + X_L^2}}, with R ≈ 0 for the choke. And the average power is

P=VrmsIrmscos⁡ϕP = V_{rms}I_{rms}\cos\phi

with φ = 90° for a pure inductor, so P = 0. But the source is still supplying current! Where does that energy go? It cannot just vanish, I am suffering.

Also two connected doubts:

  1. Why can't the same choke be used on a DC supply to cut down the current?
  2. For the transformer, I get VpIp=VsIsV_pI_p = V_sI_s for an ideal one, but real ones are not 100% efficient. What are the losses, and how are they reduced? My teacher listed four names and I forgot two of them 💀
WhatsAppPost on X

7 answers & replies

Sign in to join the conversation.

  • [+]Nisha Verma12thSample· 1mo ago

    Nothing vanishes, it's borrowed and given back. In an inductor, the current rises in a quarter cycle and energy gets stored in the magnetic field (12LI2\tfrac12 LI^2). In the next quarter the field collapses and energy goes back to the source. Over one full cycle:

    p=vi=V0I0sin⁡ωtcos⁡ωt=12V0I0sin⁡2ωtp = vi = V_0I_0\sin\omega t\cos\omega t = \tfrac12 V_0I_0\sin2\omega t

    whose average over a cycle is zero. In a resistor the energy never comes back, it leaves as heat. So the choke "limits" the current by reactance and just shuffles energy.

    • [+]Pooja Iyer12thSample· 1mo agoAuthor

      ahhh so the source gives energy to the field and the field gives it back, like a loan. 🥹 that finally makes sense. cos φ = 0 is "no net energy used", not "no current".

      • [+]Nisha Verma12thSample· 1mo ago

        yep, and that's why we call the current there "wattless current". it flows but its average power is zero.

  • [+]Kavya NaikDropperSample· 1mo ago

    Another way to see why the choke is "free": in a series L–R circuit the voltage across the resistor and across the inductor are 90° out of phase, so they don't add up simply. V2=VR2+VL2V^2 = V_R^2 + V_L^2. A choke takes up most of the supply voltage as VLV_L, and that part of the voltage is in quadrature with the current, so it does no net work. A resistor in the same place would take up its share as VRV_R, which is in phase with the current, so it burns I2RI^2R all the time. Same drop in voltage, very different bills.

  • [+]Mehak AroraDropperSample· 1mo ago

    Your DC doubt, Pooja: an inductor opposes only changes in current. For steady DC, ω=0\omega = 0 so XL=ωL=0X_L = \omega L = 0 and the only opposition left is the small resistance of the wire. A choke on DC would basically be a short circuit and get very hot. That's why choke is only for AC (the current keeps changing so L keeps opposing).

    (Pooja, I had the same doubt in 11th. You're thinking in the right direction.)

  • [+]Farhan ShaikhDropperSample· 1mo ago

    Transformer losses, the four names:

    • Copper loss: resistance of the windings (I2RI^2R). Thick wire for the high-current side.
    • Eddy currents in the core: reduced by laminating the core (thin insulated sheets).
    • Hysteresis: repeated magnetisation and demagnetisation. Use soft iron, which has a thin B–H loop.
    • Flux leakage: not all flux links the secondary. Wind coils on top of each other on a closed core.

    The humming of a transformer is another small loss (as sound). With good design, efficiency is 95%+.

  • [+]Tushar PawarDropperSample· 1mo ago

    Why a choke instead of a resistor in a real circuit, e.g. a tube light. With a resistor in series to cut the current, a lot of power would be wasted as heat, you pay for it on the bill. With a choke the average power is nearly zero (a real one has a small resistance so a very small loss), so it controls the current cheaply. Also the mnemonic for phase: ELI the ICE man. In an inductor (L), emf (E) leads current (I).

More from Pooja Iyer