Q.An electrical device draws 2kW power from AC mains (voltage 223V (rms) =50000V). The current differs (lags) in phase by ϕ(tanϕ=−43) as compared to voltage. Find
(i) R,
(ii) XC−XL, and
(iii) IM. Another device has double the values for R, XC and XL. How are the answers affected?
Concept understanding — Power Dissipation in Resistors
Power Dissipation in Resistors
Whenever charge is driven through a resistor, electrical energy is converted into heat. The rate of this conversion is the power dissipated.
Why a Resistor Heats Up
Inside a resistor, drifting electrons repeatedly collide with the vibrating lattice ions. Each collision transfers kinetic energy to the lattice, raising its temperature. The source (battery or AC supply) continually does work to keep the current flowing, and that work reappears as heat. This is Joule heating.
The Power Formulas (DC)
The power delivered to any device carrying current I across a potential difference V is
P=VI
For an ohmic resistor V=IR, so this can be written in three equivalent forms:
P=VI=I2R=RV2
The SI unit is the watt (W), where 1W=1J s−1.
Which form to use depends on what is fixed:
Series elements share the same current, so P=I2R shows the larger resistor dissipates more.
Parallel elements share the same voltage, so P=V2/R shows the smaller resistor dissipates more.
The total heat produced in time t is Q=Pt=I2Rt — Joule's law of heating.
Power Dissipation with AC
With alternating current the instantaneous power p(t)=i2(t)R fluctuates, but a resistor still only dissipates energy (it never returns any). The average power over a cycle is written with root-mean-square values:
Pavg=Irms2R=RVrms2=VrmsIrms
where for a sinusoid Irms=Im/2 and Vrms=Vm/2. This is precisely why rms values are defined: an AC of rms value Irms heats a resistor at the same average rate as a steady DC of value Irms.
Important
A pure resistor has power factor 1 — voltage and current are in phase, so all the power supplied is dissipated. In inductors and capacitors, by contrast, the average dissipated power is zero; energy is only stored and returned.
Worked Example
A 100Ω resistor carries a current of 0.5A. …
Why this formula?
Power Dissipation in Resistors — Why the Formula Holds
Let's build this from first principles. The goal is to understand why a resistor dissipates power as heat, and how the formula P=I2R (and its equivalents) arise naturally.
1. What is "Power" in an Electrical Circuit?
Power is the rate of energy transfer — how much energy is converted from one form to another per unit time.
In a resistor, electrical energy is converted into heat (thermal energy).
The fundamental definition of electrical power is:
P=V⋅I
where:
P = power (watts, W)
V = voltage across the component (volts, V)
I = current through the component (amperes, A)
Why this definition?
Voltage is energy per unit charge (V=qW), and current is charge per unit time (I=tq). Multiplying them gives energy per unit time — exactly power.
2. How Does a Resistor Behave? — Ohm's Law
A resistor obeys Ohm's Law:
V=I⋅R
where R is resistance (ohms, Ω). This is an empirical law — it describes how real resistors behave: the voltage across them is proportional to the current through them.
3. Deriving the Power Dissipation Formulas
We start with P=VI and substitute Ohm's Law in two ways.
Case A: Express power in terms of I and R
Replace V with IR:
P=(IR)⋅I=I2R
Interpretation:
For a fixed resistance, power grows with the square of current.
Doubling current quadruples the heat generated — this is why high currents cause wires to overheat.
Case B: Express power in terms of V and R
Replace I with RV:
P=V⋅(RV)=RV2
Interpretation:
For a fixed voltage, power is inversely proportional to resistance.
A low-resistance resistor (like a short circuit) dissipates huge power at a given voltage — that's why short circuits are dangerous.
4. The Physical "Why" — Energy Conversion at the Atomic Level
Why does this energy turn into heat?
Electrons moving through a resistor collide with the atoms of the material.
Each collision transfers kinetic energy from the electron to the atom, making the atom vibrate more — i.e., heating up the resistor.
The rate at which this energy is lost by the electrons (and gained by the lattice) is exactly P=I2R.
Using the exact given value Vrms=50000V=1005V throughout, the first device has R=16Ω, XC−XL=−12Ω, and peak current IM=510≈15.81A. Doubling R, XC and XL leaves the phase angle unchanged but halves the current and power: IM′=2510≈7.91A and P′=1000W.
Why this approach works
The real power drawn by an AC circuit is dissipated only in its resistive part; the phase lag ϕ between current and voltage fixes the ratio of net reactance to resistance. Given the power, the rms voltage, and tanϕ, all three quantities R, XC−XL, and the peak current IM follow directly.
P=VrmsIrmscosϕ,P=Irms2R,tanϕ=RXC−XL
Since the current lags the voltage, the circuit is net inductive; the given tanϕ=−43 carries this sign directly (XC−XL is negative because XL>XC).
Step-by-step solution
1. Find cosϕ from tanϕ.
cosϕ=1+tan2ϕ1=1+1691=16251=54
2. Find Irms from the power equation.
Using the exact given value Vrms=50000V=1005V (rather than the rounded 223V):
Method: Solving AC "Power Triangle" Problems (Given Power, RMS Voltage, and Phase Angle)
This method applies to any question that gives the power drawn, the rms supply voltage, and the phase angle (or tanϕ) of an AC circuit, and asks for the resistance, net reactance, and/or peak current — plus how scaling every element affects the result.
Steps
Step 1: Get cosϕ from tanϕ
If given tanϕ=a/b, use the right-triangle relationship (hypotenuse =a2+b2):
cosϕ=1+tan2ϕ1
Keep the sign convention in mind: check whether the question describes current lagging or leading before assigning signs to the reactance terms later.
Step 2: Find Irms from the real-power equation
P=VrmsIrmscosϕ⇒Irms=VrmscosϕP
Use the EXACT given value of Vrms (not a rounded version) if the problem supplies one, to avoid compounding rounding error through the rest of the solution.
Step 3: Find R from P=Irms2R
R=Irms2P
This works because only the resistive part of the circuit actually dissipates real power.
Step 4: Find the net reactance and the peak current …