Q.(a) The peak voltage of an ac supply is 300 V. What is the rms voltage?
Concept understanding — RMS and Peak Value
Why We Need a New Measure
When you push a DC current through a resistor, the power is constant — P=I2R, and the heating is steady. But an AC current keeps changing direction and magnitude. At one instant it's +I0, a moment later it's zero, then −I0. If you simply averaged the current over time, you'd get zero — because the positive and negative halves cancel. That's useless for telling you how much heat the resistor actually feels.
So we need a single number that captures the effective heating power of an alternating current. That number is the RMS value.
The Intuition: Squaring Fixes the Sign Problem
Heat depends on I2, not on I. Squaring the current makes every instant positive — a negative current squared gives the same heat as a positive one of the same magnitude. So instead of averaging the current (which gives zero), we average the square of the current, then take the square root to get back to a current-like number. That's the root-mean-square: Root of the Mean of the Square.
For a sinusoidal current i(t)=I0sin(ωt), the square is I02sin2(ωt). The average of sin2 over a full cycle is exactly 1/2. So:
mean of i2=I02×21
Then:
Irms=2I02=2I0
Irms=2I0andVrms=2V0
The Physical Meaning
If you take a resistor and pass a sinusoidal current of peak value I0 through it, the average power dissipated is exactly the same as if you passed a steady DC current of I0/2 through it. That's why RMS is called the "equivalent DC" value.
When you see "230 V AC" on a household outlet, that 230 V is the RMS voltage. The peak voltage is 230×2≈325 V. The wire insulation has to handle 325 V peaks, but the heating effect is the same as 230 V DC.
Peak Value
The peak value I0 (or V0) is simply the maximum instantaneous value the waveform reaches. For a sine wave, it's the amplitude. The RMS value is always smaller than the peak — by a factor of 2 for a pure sine wave.
The 2 factor applies only to sinusoidal waveforms. For a square wave, Irms=I0; for a triangular wave, Irms=I0/3. Never blindly use /2 unless you know the waveform is sinusoidal.
Summary
| Quantity | Symbol | Meaning |
|---|---|---|
| Peak current | I0 | Maximum instantaneous current |
| RMS current | Irms=I0/2 | Equivalent DC that gives same heating |
| Peak voltage | V0 | Maximum instantaneous voltage |
| RMS voltage | Vrms=V0/2 | Equivalent DC voltage for same power |
The core idea: RMS converts an alternating quantity into a steady DC equivalent for power calculations. It's the square root of the average of the square — nothing more, nothing less.
RMS and peak value calculations open the NCERT Class 12 Physics chapter on Alternating Current, and 'RMS value formula class 12 physics' or 'AC RMS and peak value important questions' are frequently searched by board and JEE Main aspirants. Because household AC ratings are always quoted as RMS values, this concept also shows up in applied, real-world exam questions.
Concept: RMS and peak values in AC circuits — for a sinusoidal waveform, the RMS value is 1/2 times the peak value.
(a)
Peak voltage V0=300 V.
RMS voltage is given by Vrms=2V0.
So Vrms=2300=1502≈212.1 V.
(b)
RMS current Irms=10 A.
Peak current I0=Irms×2.
So I0=102≈14.14 A.
- The rms voltage is 1502 V (≈ 212.1 V).
- The peak current is 102 A (≈ 14.14 A).
For a sinusoidal AC waveform, the rms value is the peak divided by 2, and the peak value is the rms multiplied by 2.
- Vrms=2300≈212 V
- I0=102≈14.1 A
Why rms and peak are linked by 2
When we say "AC voltage" or "AC current" in everyday use, we almost always mean the rms (root-mean-square) value. That’s because rms gives the equivalent DC value that would deliver the same power to a resistor. For a sinusoidal waveform — the standard shape of mains AC — the relationship is fixed:
Vrms=2V0,Irms=2I0
where V0 and I0 are the peak (maximum instantaneous) values.
The factor 2 comes from averaging the square of a sine wave over a cycle. It’s not an approximation — it’s exact for a pure sine wave.
(a) Peak voltage given, find rms voltage
1. The peak voltage is V0=300 V.
2. The rms voltage is:
Vrms=2V0=2300 V
3. Rationalise or compute numerically:
2300=300×22=1502≈150×1.414=212.1 V
So the rms voltage is about 212 V.
A common mistake is to multiply by 2 instead of dividing. Remember: peak is larger than rms, so to go from peak to rms you divide by 2.
(b) rms current given, find peak current
1. The rms current is Irms=10 A.
2. Rearranging the formula:
I0=Irms×2=102 A
3. Numerically:
10×1.414=14.14 A
So the peak current is about 14.1 A.
If you ever forget which way the factor goes, think of a 230 V mains supply — its peak is about 325 V. Since 325 > 230, peak is always larger. So:
rms → peak: multiply by 2
peak → rms: divide by 2
- The rms voltage is 1502 V≈212 V.
- The peak current is 102 A≈14.1 A.
Method: Peak–RMS Conversion for Sinusoidal AC
This method uses the fixed relationship between peak and RMS values for a pure sinusoidal waveform. The key formulas are:
- Vrms=2V0
- I0=Irms×2
Where V0 and I0 are the peak (maximum) values.
(a) Peak voltage → RMS voltage
Step 1: Identify the given peak voltage.
V0=300 V
Step 2: Apply the conversion formula.
Vrms=2V0=2300
Step 3: Simplify (rationalise if needed).
Vrms=2300×22=23002=1502
Step 4: Compute numerical value (exam-ready).
Vrms≈150×1.414=212.1 V
Answer: 212.1 V (or 1502 V)
(b) RMS current → Peak current
Step 1: Identify the given RMS current.
Irms=10 A
Step 2: Apply the reverse conversion formula.
I0=Irms×2=10×2
Step 3: Compute numerical value.
I0≈10×1.414=14.14 A
Answer: 14.14 A (or 102 A)
Why this works (concept check)
- For a sinusoidal AC, the RMS value is the DC equivalent that produces the same average power dissipation in a resistor.
- The factor 2 comes from averaging the square of sin(ωt) over one cycle.
- Important: These formulas are valid only for pure sine waves — not for square waves, triangular waves, or distorted AC.
Here are the common mistakes students make when solving problems on Power Dissipation in Resistors (specifically for AC RMS and peak values), along with clear ways to avoid each.
Mistake 1: Confusing the formula for RMS voltage and peak voltage
The Mistake
Students often write:
Vrms=2V0orVrms=V0×2
but mix them up — using the wrong one for the given data.
Why it happens
They memorise the formula without understanding the relationship:
- RMS is smaller than peak (since 21≈0.707).
- Peak is larger than RMS (by factor 2≈1.414).
How to avoid
Always ask: “Is the given value the peak or the RMS?”
- If given peak → divide by 2 to get RMS.
- If given RMS → multiply by 2 to get peak.
For part (a):
Given V0=300 V (peak).
Correct:
Vrms=2300≈212.1 V
Mistake 2: Forgetting to square-root or square incorrectly
The Mistake
Some students write:
Vrms=2V0orVrms=2V0but then square it again
Why it happens
They confuse RMS with average power formulas (where P=RVrms2).
How to avoid
Remember: RMS is root mean square — the “root” part means you take the square root at the end.
- For a sine wave: Vrms=2V0 (no extra squaring).
- Only square when calculating power, not when converting peak ↔ RMS.
Mistake 3: Using the same formula for current and voltage incorrectly
The Mistake
Students think:
Irms=2I0andVrms=2V0
are different formulas — they are identical in form.
Why it happens
They treat current and voltage as separate “types” of problems.
How to avoid
Understand: For any sinusoidal AC quantity:
RMS=2PeakandPeak=RMS×2
It works the same for voltage and current.
For part (b):
Given Irms=10 A.
Correct:
I0=10×2≈14.14 A
Mistake 4: Forgetting units or writing wrong units
The Mistake
Writing Vrms=212.1 without “V” or writing “A” for voltage.
Why it happens
Rushing through the final answer.
How to avoid
Always include the correct unit:
- Voltage → V (volts)
- Current → A (amperes)
- Power → W (watts)
Mistake 5: Not simplifying 2 or leaving answer in improper form
The Mistake
Leaving answer as 2300 without rationalising or approximating.
Why it happens
Some students think it’s acceptable to leave a fraction with a radical in the denominator.
How to avoid
In exams, either:
- Rationalise: 2300=1502≈212.1 V
- Or give decimal to 1–2 decimal places (as per question requirement).
Quick Summary Table
| Mistake | How to Avoid |
|---|---|
| Wrong formula (peak ↔ RMS) | Ask: “Given peak or RMS?” then divide or multiply by 2 |
| Extra squaring | RMS already includes square root — don’t square again |
| Treating current/voltage differently | Same formula for both |
| Missing units | Always write V or A |
| Not simplifying | Rationalise or give decimal |
Final correct answers for reference:
- Vrms=2300≈212.1 V
- I0=10×2≈14.14 A
- COMEDK 2023Set 2023-E1 markMCQQ.220 V ac is more dangerous than 220 V dc Why? (A) The peak value of ac is greater than the given value of dc (B) Shock received from ac is always repulsive (C) The frequency of ac is more than that of dc (D) The speed of ac is more than that of dc
›Reveal solutionSolution
(The other options are not physical: shock from a.c. is not 'always repulsive', d.c. has zero frequency but that is not the reason, and 'speed of ac/dc' is meaningless here.)
Concept: an a.c. supply is quoted by its RMS value, but the instantaneous voltage swings up to the PEAK value.
For 220 V a.c. (rms):
V_peak = sqrt2 x V_rms = 1.414 x 220 = 311 V.
For 220 V d.c. the voltage is steady at 220 V.
So the a.c. mains repeatedly reaches about 311 V - roughly 1.4 times the d.c. value - and it is this higher peak that drives a larger peak current through the body, making 220 V a.c. more dangerous.
(The other options are not physical: shock from a.c. is not 'always repulsive', d.c. has zero frequency but that is not the reason, and 'speed of ac/dc' is meaningless here.)
✓Final answerThe correct option is (A) — The peak value of ac is greater than the given value of dc
ANSWER: A
- COMEDK 2022Set 20221 markMCQQ.A DC ammeter and a hot wire ammeter are connected to a circuit in series. When a direct current is passed through circuit, the DC ammeter shows 6 A. When AC current flows through circuit, what is the average readings in DC ammeter and the AC ammeter, if DC and AC currents flows simultaneously through the circuit? (A) DC = 6 A, AC = 10 A (B) DC = 3 A, AC = 5 A (C) DC = 5 A, AC = 8 A (D) DC = 2 A, AC = 3 A
›Reveal solutionSolution
So DC = 6 A, AC (hot-wire) = 10 A.
Concept: A moving-coil DC ammeter responds to the average (mean) current; a hot-wire ammeter responds to the rms current (it is heat-operated, ∝ i²).
With DC alone the DC meter reads 6 A → I_dc = 6 A. With AC alone the hot-wire meter reads the rms value of the AC — from the option set this is 8 A.
Now pass both together: i(t) = I_dc + i_ac(t).
DC ammeter (average): ⟨i⟩ = I_dc + ⟨i_ac⟩ = 6 + 0 = 6 A (an AC current averages to zero).
Hot-wire ammeter (rms):
⟨i²⟩ = ⟨(I_dc + i_ac)²⟩ = I_dc² + 2I_dc⟨i_ac⟩ + ⟨i_ac²⟩ = 6² + 0 + 8² = 36 + 64 = 100
I_rms = √100 = 10 A.
So DC = 6 A, AC (hot-wire) = 10 A.
✓Final answerThe correct option is (A) — DC = 6 A, AC = 10 A
ANSWER: A
- COMEDK 2022Set 20221 markMCQQ.The AC voltage across a resistance can be measured using a (A) hot wire voltmeter (B) moving coil galvanometer (C) potential coil galvanometer (D) moving magnetic galvanometer
›Reveal solutionSolution
[!TLDR]
AC needs an instrument whose reading does not depend on current direction; the hot-wire voltmeter uses the heating effect and measures the RMS AC voltage.
Concept
This CBSE Class 12 Alternating Current idea distinguishes instruments by what they respond to. A moving-coil galvanometer measures the mean value of current; since the mean of a symmetric AC is zero, it reads zero for AC. A hot-wire instrument depends on I2R heating, which is always positive regardless of direction, so it works for both AC and DC.
Solution
- Moving-coil (and moving-magnet) galvanometers give a deflection proportional to the average current, which vanishes over an AC cycle, so options (B) and (D) cannot measure AC.
- Option (C) 'potential coil galvanometer' is not a standard AC-measuring instrument for this purpose.
- A hot-wire voltmeter passes the current through a thin wire; the wire heats up by I2R and expands, moving the pointer. Because heating is independent of the current's direction, it registers AC (its RMS value) as well as DC.
[!ANSWER]
(A) hot wire voltmeter
NoteThis solution was worked out by our team and independently cross-checked by a second solve. The official answer key on record for this question could not be confirmed, so please cross-verify with the official paper where possible.
- COMEDK 2021Set 2021-B1 markMCQQ.A 20 ohm electric heater is connected to a 220 V, 60 Hz mains supply. The peak value of electric current flowing in the circuit is (A) 22 A (B) 5.5 A (C) 11 A (D) 15.55 A
›Reveal solutionSolution
Irms=220/20=11 A, peak =2×11≈15.55 A.
For a purely resistive heater, the rms current is
Irms=RVrms=20220=11 A.
The peak (maximum) value of an AC current is 2 times the rms value:
I0=2Irms=1.414×11≈15.55 A.
✓Final answerThe correct option is (D) — 15.55 A
- COMEDK 2021Set 2021-B1 markMCQQ.A generator produces a voltage that is given by V=200sin314t where t is in seconds. The frequency and rms voltage are (A) 50 Hz, 100 V (B) 157 Hz, 141 V (C) 157 Hz, 100 V (D) 50 Hz, 141 V
›Reveal solutionSolution
f=314/2π=50 Hz; Vrms=200/2=141 V.
Comparing V=200sin(314t) with V=V0sin(ωt):
- Angular frequency ω=314 rad/s, so
f=2πω=6.283314≈50 Hz.
- Peak voltage V0=200 V, so
Vrms=2V0=1.414200≈141 V.
✓Final answerThe correct option is (D) — 50 Hz, 141 V
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