Suppose a charge \( Q \) flows through a conductor in time \( t \).
By definition, current is the amount of charge flowing per unit time:
\[ I = \frac{Q}{t} \]
If the flow is uniform:
\[ Q = It \]
This relation is widely used in numerical problems.
Current, Resistance, Circuits, and Electrical Power
From Ohm's Law to Household Wiring — Decode Every Circuit
Electricity is the highest-weightage physics chapter in Class X, contributing 14–16 marks in CBSE Boards. Ohm's Law, series and parallel resistance, and electrical power calculations are guaranteed formula questions. Circuit diagram drawing is a standard 3-mark question. NTSE includes complex circuit analysis and energy calculation problems. This is the most calculation-intensive science chapter.
Parallel combination is the most common calculation error — use 1/R = 1/R₁ + 1/R₂ and then invert. For power problems: if voltage is constant across devices (parallel in household), use P = V²/R; if current is constant (series), use P = I²R. Energy bill: multiply power (kW) × time (hours) = kWh, then multiply by rate. Always draw the circuit before calculating. Time investment: 5–6 days.
Suppose a charge \( Q \) flows through a conductor in time \( t \).
By definition, current is the amount of charge flowing per unit time:
\[ I = \frac{Q}{t} \]
If the flow is uniform:
\[ Q = It \]
This relation is widely used in numerical problems.
A wire carries a steady current. If the amount of charge flowing doubles while time remains constant, what happens to current?
Analysis:
\[ I = \frac{Q}{t} \]
If \( Q \) doubles and \( t \) remains constant:
\[ I \propto Q \]
Conclusion: Current also doubles.
The conventional direction of current is from the positive terminal to the negative terminal of a battery, although electrons actually move in the opposite direction.
Circuit diagrams use standard symbols to represent electrical components, simplifying analysis and design.
Let charge \(Q\) flow through a conductor in time \(t\). By definition,
\[ I = \frac{Q}{t} \]
Rearranging:
\[ Q = It \]
This relation is crucial in numerical applications.
SI unit of current is ampere (A), named after :contentReference[oaicite:0]{index=0}.
\[ 1\,A = \frac{1\,C}{1\,s} \]
A circuit is connected but the switch is open. A student claims current still flows due to battery. Is the student correct?
Analysis:
Current requires a closed path. An open switch breaks the circuit.
Conclusion: No current flows. The student is incorrect.
Final Answer: \( Q = 300 \, C \)
This means that a total charge of 300 coulombs passes through the filament in 10 minutes. It indicates continuous movement of a large number of electrons through the circuit.
Final Answer: \( Q = 300 \, C \)
A charge of 300 coulombs passes through the bulb in 20 minutes, indicating continuous flow of electrons driven by the potential difference.
Work done \( W \) is required to move charge \( Q \) between two points.
By definition of potential difference:
\[ V = \frac{W}{Q} \]
Rearranging:
\[ W = VQ \]
This equation is frequently used in numerical problems and energy calculations.
SI unit of potential difference is volt (V), named after :contentReference[oaicite:0]{index=0}.
\[ 1\,V = \frac{1\,J}{1\,C} = 1\,J\,C^{-1} \]
This means one volt is the potential difference when 1 joule of work is done to move 1 coulomb of charge.
Final Answer: \( W = 24 \, J \)
This means 24 joules of electrical energy is required to move 2 coulombs of charge across the given potential difference. This energy may be converted into heat, light, or other forms depending on the circuit element.
Final Answer: \( W = 20 \, J \)
Moving the charge from a lower potential (118 V) to a higher potential (128 V) requires energy. Hence, 20 joules of work is done on the charge.
Always calculate potential difference first when two potentials are given. Direct substitution without finding difference is a common mistake.
\[ V \propto I \quad \Rightarrow \quad V = IR \]
\[ I = \frac{V}{R} \]
The graph between voltage (V) and current (I) is a straight line passing through the origin. The slope of the graph gives resistance.
Experimentally:
\[ R \propto l \quad \text{and} \quad R \propto \frac{1}{A} \]
Combining:
\[ R \propto \frac{l}{A} \]
Introducing proportionality constant (resistivity \( \rho \)):
\[ R = \rho \frac{l}{A} \]
Resistance increases with length because electrons travel a longer path and collide more frequently with atoms.
\[ R \propto l \]
Resistance decreases with increase in area because a thicker wire provides more paths for electron flow.
\[ R \propto \frac{1}{A} \]
Different materials have different resistivities:
For metals, resistance increases with temperature due to increased atomic vibrations.
For semiconductors, resistance decreases with temperature (important concept).
(a) How much current will an electric bulb draw from a 220 V source,
if the resistance of the bulb filament is 1200 Ω?
(b) How much current will an electric heater coil draw from a 220 V source,
if the resistance of the heater coil is 100 Ω?
(a) For bulb:
\[ I = \frac{220}{1200} \approx 0.18 \, A \]
(b) For heater:
\[ I = \frac{220}{100} = 2.2 \, A \]
Final Answers:
(a) \( 0.18 \, A \)
(b) \( 2.2 \, A \)
The heater draws much more current than the bulb because it has much lower resistance.
This explains why heaters produce more heat—they allow larger current flow.
In series combination, resistors are connected end-to-end such that the same current flows through each.
\[ R_s = R_1 + R_2 + R_3 + \cdots \]
\[ V = V_1 + V_2 + V_3 \]
\[ \begin{aligned} V &= IR,\\ V_1 &= IR_1,\\ V_2 &= IR_2,\\ V_3 &= IR_3 \end{aligned} \]
\[ \begin{aligned} IR &= IR_1 + IR_2 + IR_3\\ \Rightarrow R_s &= R_1 + R_2 + R_3 \end{aligned} \]
In parallel combination, resistors are connected across the same two points, providing multiple paths for current.
\[ \frac{1}{R_p} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} \]
\[ I = I_1 + I_2 + I_3 \]
\[ \begin{aligned} I &= \frac{V}{R_p},\\\\ I_1 &= \frac{V}{R_1},\\\\ I_2 &= \frac{V}{R_2},\\\\ I_3 &= \frac{V}{R_3} \end{aligned} \]
\[ \begin{aligned} \frac{V}{R_p} &= \frac{V}{R_1} + \frac{V}{R_2} + \frac{V}{R_3}\\\\ \Rightarrow \frac{1}{R_p} &= \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} \end{aligned} \]
| Feature | Series Circuit | Parallel Circuit |
|---|---|---|
| Current |
Same through all components \( I = I_1 = I_2 = \dots \) |
Divides among branches \( I = I_1 + I_2 + \dots \)] |
| Voltage |
Divides across components \( V = V_1 + V_2 + \dots \) |
Same across each branch \( V = V_1 = V_2 = \dots \) |
| Equivalent Resistance |
Increases \( R = R_1 + R_2 + \dots \) |
Decreases \( \frac{1}{R} = \frac{1}{R_1} + \frac{1}{R_2} + \dots \) |
| Path for Current | Only one path | Multiple paths |
| If one component fails | Whole circuit stops | Other branches may still work |
Three resistors \( R_1 = 5 \, \Omega \), \( R_2 = 10 \, \Omega \), and \( R_3 = 30 \, \Omega \)
are connected in parallel to a 12 V battery. Calculate:
(a) current through each resistor
(b) total current in the circuit
(c) equivalent resistance of the circuit
This matches the calculated total current, confirming correctness.
In a circuit, resistors \( R_1 = 10 \, \Omega \), \( R_2 = 40 \, \Omega \),
\( R_3 = 30 \, \Omega \), \( R_4 = 20 \, \Omega \), and \( R_5 = 60 \, \Omega \)
are connected as shown. A 12 V battery is applied.
Calculate:
(a) total resistance
(b) total current in the circuit
Work done in moving charge \(\small Q \) through potential difference \(\small V \):
\[ \small W = VQ \]
Power is rate of doing work:
\[\small P = \frac{W}{t} = \frac{VQ}{t} \]
Since \(\small I = \frac{Q}{t} \),
\[\small
P = VI
\]
Energy supplied in time \( t \):
\[
H = Pt = VIt
\]
Using Ohm’s Law \( V = IR \):
\[
H = I^2 R t
\]
Also, using \( I = \frac{V}{R} \):
\[
H = \frac{V^2}{R} t
\]Heat Produced
Electrical energy is measured in kilowatt-hour (kWh), also called a unit.
\[\small 1 \, kWh = 3.6 \times 10^6 \, J \]
Question: Why are heating devices made of high resistance materials?
Answer: Because heat produced is proportional to resistance (\( H \propto R \)).
At maximum heating, resistance is lower, allowing more current to flow. At minimum heating, resistance increases, reducing current and heat output.
100 J of heat is produced each second in a 4 Ω resistor. Find the potential difference across the resistor.
Uses a nichrome heating element to generate heat. A thermostat maintains constant temperature.
Converts electrical energy into heat for warming air or water using resistive coils.
Tungsten filament glows when heated to high temperature due to current flow.
A safety device that melts when excess current flows, breaking the circuit.
Used in electric furnaces, welding, and metal cutting where high temperature is required.
Devices like electric stoves, kettles, and induction cooktops use heating effect for cooking.
SI unit: Watt (W)
\[ 1 \, W = 1 \, \frac{J}{s} \]
Larger units:
Energy consumed:
\[\small E = P \times t \]
Commercial unit:
\[\small 1 \, kWh = 3.6 \times 10^6 \, J \]
A comprehensive, interactive learning engine for deep conceptual mastery
Electric current is the rate of flow of electric charge. Charge is carried by electrons in metallic conductors. SI unit: Ampere (A).
Potential difference drives current between two points. EMF is the work done per unit charge by the source of electricity. Unit: Volt (V).
At constant temperature, current through a conductor is directly proportional to potential difference across it: V = IR.
Resistance opposes current flow. Resistivity (ρ) is a property of the material, independent of shape. R = ρl/A.
Series: same current, voltages add. Parallel: same voltage, currents add. Combined resistance rules differ for each arrangement.
Power P = VI = I²R = V²/R. Energy = Power × Time. Commercial unit is kilowatt-hour (kWh). 1 kWh = 3.6 × 10⁶ J.
| Quantity | Symbol | SI Unit | Symbol |
|---|---|---|---|
| Electric Charge | Q | Coulomb | C |
| Electric Current | I | Ampere | A |
| Potential Difference | V | Volt | V |
| Resistance | R | Ohm | Ω |
| Resistivity | ρ | Ohm·metre | Ω·m |
| Power | P | Watt | W |
| Energy | W | Joule | J |
| Time | t | Second | s |
| Length | l | Metre | m |
| Area | A | Square metre | m² |
Current is the net charge flowing past a cross-section per unit time. 1 A = 1 C/s.
Valid when temperature and physical conditions are constant. Ohmic conductors follow this linearly.
R ∝ l and R ∝ 1/A. Resistivity depends only on material and temperature.
1 Volt = 1 Joule per Coulomb. Represents energy supplied per unit charge.
Same current flows through each. Total resistance is always greater than the largest individual resistor. Voltages add up.
Same voltage across each. Total resistance is less than the smallest individual resistor. Currents add up.
Product over sum formula — a quick shortcut when exactly two resistors are in parallel.
Rate of doing work or energy consumed per unit time. 1 W = 1 J/s.
I²R is used when current is known. V²/R when voltage is known. Both derived from P=VI and Ohm's Law.
Heat produced in a resistor equals electrical energy dissipated. Commercial unit: kWh. 1 kWh = 3.6 × 10⁶ J.
The commercial unit of electrical energy. Electricity bills are calculated in kWh (1 unit = 1 kWh).
Draw a triangle: V on top, I and R at the bottom. Cover what you want — the remaining gives the formula. Cover V → V=IR; Cover I → I=V/R; Cover R → R=V/I.
In series: current is same, voltage divides. In parallel: voltage is same, current divides. If asked about "same current everywhere" — it's series; "same voltage everywhere" — it's parallel.
Equivalent parallel resistance is always less than the smallest resistor. Use this to instantly check if your answer is plausible!
Remember "PIE": P = I×E (E = Voltage V). Then P = I²R and P = V²/R follow by substituting V=IR into PIE.
Resistivity (ρ) is a material property — it changes with temperature but NOT with dimensions. Resistance (R) changes with both material AND dimensions (length and area).
1 kWh = 1000 W × 3600 s = 3,600,000 J = 3.6 × 10⁶ J. Memorise this conversion — it appears frequently in energy-cost problems.
Conventional current flows from + to − (positive terminal to negative). Electrons actually flow from − to + (opposite direction). Remember: "Conventional Current goes from Positive to Negative — like C for Conventional, C for anode (positive Carbon rod)."
R = ρl/A. If l doubles → R doubles. If A doubles → R halves. If a wire is stretched to double its length, its area halves (volume is constant), so R becomes 4 times the original!
Plot V vs I: if it's a straight line through the origin → Ohmic conductor. Non-linear (like a diode or bulb) → non-Ohmic. Temperature affects the slope (resistance).
Say "I-square-R-t" as "Ice-art" → Heat = I²Rt. More current → exponentially more heat (squared relationship). This is why thick wires are used for high-current circuits.
Students apply the addition rule to parallel circuits and the reciprocal rule to series — a very common slip.
Students correctly compute 1/R_total but forget to invert it to get R_total.
Choosing P = V²/R when only current and resistance are given, or vice versa.
Using watts and hours together without converting to consistent units.
Ohm's Law applies only to Ohmic conductors at constant temperature. Non-Ohmic devices (diodes, bulb filaments) have variable resistance.
Saying "copper has low resistance" when one should say "copper has low resistivity." Resistance depends on dimensions; resistivity does not.
Saying electrons flow from positive to negative terminal inside the external circuit.
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