When the terminals of a cell are connected to a conductor of resistance R, an electric current flows through t

Question

\varepsilon

(i) Choose the incorrect statement : (A) The potential difference (V) between the two terminals of a cell in a closed circuit is always less than its emf (

\varepsilon

), during discharge of the cell. (B) The internal resistance of a cell decreases with the decrease in temperature of the electrolyte. (C) When current is drawn from the cell then

V = \varepsilon - Ir

. (D) The graph between potential difference between the two terminals of the cell (V) and the current (I) through it is a straight line with a negative slope.

(ii) Two cells of emfs

2{\cdot}0

V and

6{\cdot}0

V and internal resistances

0{\cdot}1\ \Omega

and

0{\cdot}4\ \Omega

respectively, are connected in parallel. The equivalent emf of the combination will be : (A)

2{\cdot}0

V (B)

2{\cdot}8

V (C)

6{\cdot}0

V (D)

8{\cdot}0

(iii) Dipped in the solution, the electrode exchanges charges with the electrolyte. The positive electrode develops a potential

V_+

(

V_+ > 0

), and the negative electrode develops a potential

-(V_-)

(

V_- \geq 0

), relative to the electrolyte adjacent to it. When no current is drawn from the cell then : (A)

\varepsilon = V_+ + V_- > 0

(B)

\varepsilon = V_+ - V_- > 0

(C)

\varepsilon = V_+ + V_- < 0

(D)

\varepsilon = V_+ + V_- = 0

(iv)

(a) Five identical cells, each of emf 2 V and internal resistance

0{\cdot}1\ \Omega

are connected in parallel. This combination in turn is connected to an external resistor of

9{\cdot}98\ \Omega

. The current flowing through the resistor is : (A)

0{\cdot}05

A (B)

0{\cdot}1

A (C)

0{\cdot}15

A (D)

0{\cdot}2

(OR)

(b) Potential difference across a cell in the open circuit is 6 V. It becomes 4 V when a current of 2 A is drawn from it. The internal resistance of the cell is : (A)

1{\cdot}0\ \Omega

(B)

1{\cdot}5\ \Omega

(C)

2{\cdot}0\ \Omega

(D)

2{\cdot}5\ \Omega

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Part (a)Concept understanding — Internal Resistance

Internal Resistance – The Battery That Fights Itself

Imagine you have a bucket of water with a tap at the bottom. When you open the tap fully, water flows out freely. But if the pipe is narrow or clogged, the flow is weaker even though the bucket is full. A battery behaves the same way: it has a "full bucket" of electrical energy (its emf, or electromotive force), but inside the battery, there is always some "clogged pipe" that resists the flow of charge. That clog is called internal resistance.

The Intuition

Every real battery is not a perfect source of voltage. If you connect a small bulb to a fresh battery, it glows brightly. But if you connect a powerful motor that draws a large current, the same battery might struggle — the voltage at its terminals drops, and the motor runs slower. Why? Because inside the battery, the chemical reactions and the materials themselves have a natural opposition to the flow of charge. This opposition is internal resistance, denoted by $r$ (or sometimes $R_{\text{int}}$ ).

Think of it this way: the battery has two "battles" to fight. First, it must push charge through the external circuit (the bulb, the motor, the wires). Second, it must push charge through its own internal structure. The harder it has to push (i.e., the larger the current), the more voltage it "loses" inside itself.

The Precise Statement

Internal resistance is the opposition to the flow of electric current offered by the materials and chemical processes inside a source of emf (like a battery, cell, or generator). It is measured in ohms ( $\Omega$ ).

For a cell or battery, the relationship between the emf ( $\mathcal{E}$ ), the terminal voltage ( $V$ ), the current ( $I$ ), and the internal resistance ( $r$ ) is given by:

V = \mathcal{E} - I r

This is the single most important equation to remember.

V = \mathcal{E} - I r

Here:

$\mathcal{E}$ is the electromotive force — the maximum voltage the battery can provide when no current flows (open circuit). Think of it as the "ideal" voltage.
$V$ is the terminal voltage — the actual voltage you measure across the battery's terminals when it is delivering current.
$I$ is the current flowing through the circuit (and therefore through the battery itself).
$r$ is the internal resistance.

The term $I r$ is the voltage drop inside the battery. It is the "price" the battery pays for delivering current.

What Happens in Different Situations?

Condition	Current $I$	Terminal Voltage $V$	Why?
Open circuit (no load)	$I = 0$	$V = \mathcal{E}$	No current means no internal drop.
Small load (e.g., a dim bulb)	Small $I$	$V \approx \mathcal{E}$	The $I r$ term is tiny.
Large load (e.g., a powerful motor)	Large $I$	$V < \mathcal{E}$ significantly	The $I r$ drop becomes noticeable.
Short circuit (wires directly across terminals)	Very large $I$	$V \approx 0$	Almost all voltage is lost inside the battery; the battery heats up and may be damaged.

Watch out

A common mistake is to think that internal resistance is a "bad" thing that can be eliminated. It cannot — every real source has some internal resistance. Even a brand new AA battery has a small $r$ (typically $0.1$ to $0.5\ \Omega$ ). Old or weak batteries have much larger $r$ , which is why they fail to power high-current devices.

Why Does Internal Resistance Matter?

Power loss inside the battery: The power dissipated as heat inside the battery is $P_{\text{loss}} = I^2 r$ . This is why batteries get warm when delivering large currents.
Maximum power transfer: There is a famous theorem (Maximum Power Transfer Theorem) that says a source delivers maximum power to an external load when the load resistance equals the internal resistance ( $R_{\text{load}} = r$ ). But this is inefficient — half the power is wasted inside the source. …

Why this formula?

Internal Resistance: Why the Key Formulas Hold

Internal resistance is a fundamental concept in real-world circuits. No battery is perfect — every practical source has some internal resistance ( $r$ ) that opposes the flow of current inside the source itself.

1. The Core Idea: A Real Battery = An Ideal Source + A Resistor

Think of a real battery as:

An ideal EMF source ( $\mathcal{E}$ ) — provides constant voltage with zero internal resistance.
A small resistor ( $r$ ) — connected in series inside the battery.

Why series? Because the current that leaves the battery must first pass through its internal material (electrolyte, electrodes), which offers resistance.

2. The Terminal Voltage Formula

When the battery delivers current $I$ to an external circuit:

The ideal source produces $\mathcal{E}$ .
The internal resistor $r$ drops some voltage: $V_{\text{drop}} = I r$ (Ohm's law).
The voltage available at the terminals ( $V$ ) is what's left:

V = \mathcal{E} - I r

Why this makes sense:

If $I = 0$ (open circuit), $V = \mathcal{E}$ — you measure the full EMF.
If $I$ increases, $V$ decreases — the internal drop grows.
If $I$ is huge (short circuit), $V \to 0$ and all voltage is lost inside.

3. The Short-Circuit Current Formula

If you connect the terminals directly (external resistance $R = 0$ ):

The only resistance in the circuit is $r$ .
By Ohm's law: $I_{\text{short}} = \frac{\mathcal{E}}{r}$

Why this holds:

The entire EMF is now dropped across $r$ alone.
This is the maximum current the battery can deliver — limited by its internal resistance.
In practice, this can damage the battery (heating, chemical damage).

4. Power Delivered to External Load

When the battery is connected to an external load $R$ :

Total circuit resistance: $R + r$
Current: $I = \frac{\mathcal{E}}{R + r}$
Power delivered to the external load ( $P_{\text{out}}$ ):

P_{\text{out}} = I^2 R = \left( \frac{\mathcal{E}}{R + r} \right)^2 R

Why this matters:

Power is not simply $\mathcal{E}^2 / R$ — because $r$ limits current. …

Part (b)Concept understanding — Internal Resistance

Internal Resistance – The Battery That Fights Itself

The Intuition

The Precise Statement

For a cell or battery, the relationship between the emf ( $\mathcal{E}$ ), the terminal voltage ( $V$ ), the current ( $I$ ), and the internal resistance ( $r$ ) is given by:

V = \mathcal{E} - I r

This is the single most important equation to remember.

V = \mathcal{E} - I r

Here:

$\mathcal{E}$ is the electromotive force — the maximum voltage the battery can provide when no current flows (open circuit). Think of it as the "ideal" voltage.
$V$ is the terminal voltage — the actual voltage you measure across the battery's terminals when it is delivering current.
$I$ is the current flowing through the circuit (and therefore through the battery itself).
$r$ is the internal resistance.

The term $I r$ is the voltage drop inside the battery. It is the "price" the battery pays for delivering current.

What Happens in Different Situations?

Condition	Current $I$	Terminal Voltage $V$	Why?
Open circuit (no load)	$I = 0$	$V = \mathcal{E}$	No current means no internal drop.
Small load (e.g., a dim bulb)	Small $I$	$V \approx \mathcal{E}$	The $I r$ term is tiny.
Large load (e.g., a powerful motor)	Large $I$	$V < \mathcal{E}$ significantly	The $I r$ drop becomes noticeable.
Short circuit (wires directly across terminals)	Very large $I$	$V \approx 0$	Almost all voltage is lost inside the battery; the battery heats up and may be damaged.

Watch out

Why Does Internal Resistance Matter?

Power loss inside the battery: The power dissipated as heat inside the battery is $P_{\text{loss}} = I^2 r$ . This is why batteries get warm when delivering large currents.
Maximum power transfer: There is a famous theorem (Maximum Power Transfer Theorem) that says a source delivers maximum power to an external load when the load resistance equals the internal resistance ( $R_{\text{load}} = r$ ). But this is inefficient — half the power is wasted inside the source. …

Why this formula?

Internal Resistance: Why the Key Formulas Hold

1. The Core Idea: A Real Battery = An Ideal Source + A Resistor

Think of a real battery as:

An ideal EMF source ( $\mathcal{E}$ ) — provides constant voltage with zero internal resistance.
A small resistor ( $r$ ) — connected in series inside the battery.

Why series? Because the current that leaves the battery must first pass through its internal material (electrolyte, electrodes), which offers resistance.

2. The Terminal Voltage Formula

When the battery delivers current $I$ to an external circuit:

The ideal source produces $\mathcal{E}$ .
The internal resistor $r$ drops some voltage: $V_{\text{drop}} = I r$ (Ohm's law).
The voltage available at the terminals ( $V$ ) is what's left:

V = \mathcal{E} - I r

Why this makes sense:

If $I = 0$ (open circuit), $V = \mathcal{E}$ — you measure the full EMF.
If $I$ increases, $V$ decreases — the internal drop grows.
If $I$ is huge (short circuit), $V \to 0$ and all voltage is lost inside.

3. The Short-Circuit Current Formula

If you connect the terminals directly (external resistance $R = 0$ ):

The only resistance in the circuit is $r$ .
By Ohm's law: $I_{\text{short}} = \frac{\mathcal{E}}{r}$

Why this holds:

The entire EMF is now dropped across $r$ alone.
This is the maximum current the battery can deliver — limited by its internal resistance.
In practice, this can damage the battery (heating, chemical damage).

4. Power Delivered to External Load

When the battery is connected to an external load $R$ :

Total circuit resistance: $R + r$
Current: $I = \frac{\mathcal{E}}{R + r}$
Power delivered to the external load ( $P_{\text{out}}$ ):

P_{\text{out}} = I^2 R = \left( \frac{\mathcal{E}}{R + r} \right)^2 R

Why this matters:

Power is not simply $\mathcal{E}^2 / R$ — because $r$ limits current. …

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Internal resistance makes $V=\varepsilon-Ir<\varepsilon$ when current flows. Answers: (i) B, (ii) B (2.8 V), (iii) A, (iv)(a) 0.2 A → D, (iv)(b) 1.0 Ω → A.

The electrolyte of a cell opposes the current just like the external resistor, so a part $Ir$ of the emf is lost inside the cell. The voltage actually available at the terminals is therefore $V=\varepsilon-Ir$ .

Part (a)

(i) Which statement is incorrect?

(A) During discharge $V=\varepsilon-Ir<\varepsilon$ — correct.
(B) "Internal resistance decreases as temperature decreases." As temperature falls, ion mobility falls, so internal resistance rises. This statement is false — it is the required answer.
(C) $V=\varepsilon-Ir$ — the standard relation, correct.
(D) $V=\varepsilon-Ir$ is linear in $I$ with slope $-r$ , a straight line of negative slope — correct.

Watch out

The trap is (B): colder electrolyte $\Rightarrow$ higher internal resistance, not lower.

(ii) Equivalent emf of two parallel cells.

For cells in parallel the equivalent emf is the conductance-weighted mean:

\varepsilon_{eq}=\frac{\varepsilon_1/r_1+\varepsilon_2/r_2}{1/r_1+1/r_2}.

With $\varepsilon_1=2.0\ \text{V},\ r_1=0.1\ \Omega,\ \varepsilon_2=6.0\ \text{V},\ r_2=0.4\ \Omega$ :

\varepsilon_{eq}=\frac{20+15}{10+2.5}=\frac{35}{12.5}=2.8\ \text{V}\quad\Rightarrow\ \textbf{(B)}.

(iii) EMF from electrode potentials.

The positive electrode sits at $+V_+$ and the negative at $-V_-$ relative to the electrolyte, so

\varepsilon=V_+-(-V_-)=V_++V_->0\quad\Rightarrow\ \textbf{(A)}.

(iv)(a) Five identical cells in parallel feeding $9.98\ \Omega$ .

Identical cells in parallel keep the same emf but divide the internal resistance: …

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Same / Similar Concept — real previous-year questions on the same or a closely similar concept, not this exact question.

Showing the 12 most recent of 23 on this concept.

CBSE 2026Set A1 markMCQ
$Q. A cell of internal resistance r is connected to an external resistance R. The current will be maximum in R, if (A) R = r/2 (B) R = r (C) R > r (D) R < r$
›Reveal solutionSolution

I = ε/(R+r); smaller R ⇒ larger current, so current is maximum for R < r (ideally R → 0).

The circuit current is $I = \dfrac{\varepsilon}{R+r}$ .

For a fixed emf ε and fixed internal resistance r, the current increases as the external resistance R decreases. Hence the current through R is maximum when R is as small as possible. Among the given choices, this corresponds t …

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CBSE 2026Set ANNUAL1 markMCQ
$Q. The electromotive force of an accumulator battery is 10 V and internal resistance 0.5Ω. The maximum electric current obtained from the battery will be$
(a) 5 A
(b) 10 A
(c) 20 A
(d) 0.05 A
›Reveal solutionSolution

The maximum current a cell can deliver is its short-circuit current, I = EMF / internal resistance.

A real battery has EMF (epsilon) and internal resistance r. When connected to an external circuit of resistance R, the current is I = epsilon/(R+r), which is largest when R = 0 (sho …

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CBSE 2026Set ANNUAL1 mark
$Q. Fill in the blank: The quantity measured across a cell without drawing any current from it, is ..... .$
›Reveal solutionSolution

The potential difference measured across a cell's terminals when no current is drawn from it equals the cell's EMF.

When current $I$ flows, the terminal voltage is $V = \varepsilon - Ir$ (less than the EMF $\varepsilon$ due to the voltage drop across internal resistance $r$ ). When no current is drawn ( $I=0$ , open circuit, e.g. measured with a …

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CBSE 2026Set ANNUAL1 markMCQ
$Q. The internal resistance of a cell depends on:$
(a) the area of the plates
(b) the distance between the plates
(c) the concentration of the electrolyte
(d) All of the above
›Reveal solutionSolution

A cell's internal resistance behaves like the resistance of the electrolyte column between its electrodes, so it depends on every geometric and chemical factor that affects that column.

Inside a cell, current flows through the electrolyte between the two electrodes. Treating the electrolyte as a conducting medium, its resistance follows the same rule as any conductor: $r=\rho\dfrac{l}{A}$ , where $\rho$ is the electrolyte's resistivity, $l$ the distance between the plates, and $A$ the area of the plates. So (i) a larger plate area $A$ gives a lower resistance (more parallel paths for current), (ii) a larger separation $l$ between plates gives a higher resistance (lon …

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CBSE 2025Set ANNUAL1 markMCQ
$Q. The maximum current that can be drawn from a cell is when$
(a) R = 0
(b) r = 0
(c) R > r
(d) r > R
›Reveal solutionSolution

Current from a cell $I = E/(R+r)$ is largest when the total resistance $(R+r)$ is smallest, i.e. when the external resistance R = 0.

For a cell of emf E and internal resistance r connected to an external resistance R, the current is

$I = \frac{E}{R+r}$

…

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CBSE 2024Set 55/5/11 markMCQ
$2\,\Omega$
›Reveal solutionSolution
A real battery has an internal resistance that causes its terminal voltage to drop when current is drawn. By analyzing the battery's behavior under two different load conditions, we can determine its internal resistance, which is $\boxed{0.5\,\Omega}$ .

A battery is not an ideal voltage source; it possesses an inherent internal resistance, denoted by $r$ . This internal resistance is effectively in series with the battery's electromotive force (EMF), $E$ . When a current $I$ is drawn from the battery through an external resistor $R$ , a voltage drop occurs across this internal resistance, equal to $Ir$ .

The voltage available across the terminals of the battery, known as the terminal voltage $V$ , is therefore less than the EMF $E$ . It is given by:
$V = E - Ir$
This terminal voltage is also the voltage across the external resistor $R$ , so $V = IR$ .

Equating these two expressions for $V$ , we get:
$IR = E - Ir$
Rearranging this equation to solve for the EMF $E$ :
$E = I(R + r)$

Formulate equations for each scenario.

We are given two distinct situations where the battery is connected to a different external resistor, resulting in a different current. We will apply the formula $E = I(R + r)$ to each case.

Scenario 1: The battery supplies a current $I_1 = 0.9\,\text{A}$ through an external resistor $R_1 = 2\,\Omega$ . Using the formula $E = I(R + r)$ :

$E = 0.9\,\text{A} \times (2\,\Omega + r)$ $E = 1.8 + 0.9r \quad \text{(Equation 1)}$
* **Scenario 2:** The battery supplies a current $I_2 = 0.3\,\text{A}$ through an external resistor $R_2 = 7\,\Omega$. Using the formula $E = I(R + r)$:
$E = 0.3\,\text{A} \times (7\,\Omega + r)$ $E = 2.1 + 0.3r \quad \text{(Equation 2)}$

Solve the system of equations for $r$ . …
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CBSE 2024Set 55/1/11 markMCQ
$6\ \text{V}$
›Reveal solutionSolution
Two cells with internal resistances in parallel drive current through each other; the terminal voltage $V_{AB}$ is found by treating each branch as a source with EMF and internal resistance, then using the parallel-source formula. The answer is $\boxed{8 \text{ V}}$ .

Why this approach works: cells with internal resistance in parallel

When two cells are connected in parallel between the same two points A and B, they don't simply "add up" like batteries in series. Each cell has an EMF (electromotive force) and an internal resistance, and they can drive current through each other. The stronger cell (higher EMF per unit resistance) will actually charge the weaker one.

The key insight: treat each branch as a source characterized by its EMF $\mathcal{E}$ and internal resistance $r$ . The terminal voltage $V_{AB}$ across the parallel combination is the voltage that appears at the terminals when both sources are connected together. This is given by the weighted average of the EMFs, where the weights are the conductances (reciprocals of internal resistances).
$V_{AB} = \frac{\frac{\mathcal{E}_1}{r_1} + \frac{\mathcal{E}_2}{r_2}}{\frac{1}{r_1} + \frac{1}{r_2}}$
This formula comes from applying Kirchhoff's laws: the current from each source adjusts so that both branches have the same terminal voltage.

Step-by-step solution

1. Identify the parameters of each branch from the circuit

Figure: two-branch circuit between A and B

Reading the circuit:

Upper branch: EMF $\mathcal{E}_1 = 12 \text{ V}$ , internal resistance $r_1 = 1 \, \Omega$

Lower branch: EMF $\mathcal{E}_2 = 6 \text{ V}$ , internal resistance $r_2 = 0.5 \, \Omega$

2. Calculate the "weighted EMFs" (EMF divided by internal resistance)

These represent the short-circuit current each source can deliver:
$\frac{\mathcal{E}_1}{r_1} = \frac{12}{1} = 12 \text{ A}$ $\frac{\mathcal{E}_2}{r_2} = \frac{6}{0.5} = 12 \text{ A}$
Interestingly, both branches have the same short-circuit current capability.

3. Calculate the sum of conductances …
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CBSE 2023Set 55/1/11 markMCQ
$8\ \text{V}$
(a) $4\ \Omega$
(b) $3\ \Omega$
(c) $2\ \Omega$
(d) $1\ \Omega$
›Reveal solutionSolution
The key idea is that the open-circuit voltage is the cell’s EMF ( $\mathcal{E} = 8\ \text{V}$ ), and the drop to $4\ \text{V}$ when $4\ \text{A}$ flows is due entirely to the voltage drop across the internal resistance $r$ . Using $V = \mathcal{E} - Ir$ , we get $r = 1\ \Omega$ , so the correct option is (d).

Every real cell behaves like a perfect EMF source $\mathcal{E}$ in series with a small internal resistance $r$ . When no current flows (open circuit), the terminal voltage equals $\mathcal{E}$ — there’s no drop across $r$ . But the moment you draw current, $r$ steals some voltage: $V_{\text{terminal}} = \mathcal{E} - I r$ . That’s the whole physics in one line.

Here, the open-circuit reading gives $\mathcal{E} = 8\ \text{V}$ . When $4\ \text{A}$ is drawn, the terminal voltage crashes to $4\ \text{V}$ . That $4\ \text{V}$ loss is $I r$ . So:

Write the terminal voltage equation:

$V = \mathcal{E} - I r$

Plug in the numbers:

$4 = 8 - (4) r$

Solve for $r$ : $4r = 8 - 4 = 4 \quad\Rightarrow\quad r = 1\ \Omega$ …
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CBSE 2023Set 55/3/11 markMCQ
$Q. Two statements are given - one labelled Assertion (A) and the other labelled Reason (R). Select the correct answer from the codes (a), (b),$
(c) and
(d) below.
(a) Both Assertion (A) and Reason (R) are true and Reason (R) is the correct explanation of the Assertion (A).
(b) Both Assertion (A) and Reason (R) are true, but Reason (R) is not the correct explanation of the Assertion (A).
(c) Assertion (A) is true, but Reason (R) is false.
(d) Assertion (A) is false and Reason (R) is also false. Assertion (A) : The internal resistance of a cell is constant. Reason (R) : Ionic concentration of the electrolyte remains same during use of a cell.
›Reveal solutionSolution
Both statements are false: a cell's internal resistance increases as the electrolyte concentration changes and ions are consumed during discharge, making the correct answer (d).

Why internal resistance matters

The internal resistance of a cell arises from the opposition to ion flow within the electrolyte and at the electrode-electrolyte interfaces. If the cell were an ideal voltage source, it would have zero internal resistance. Real cells, however, have finite $r$ that affects the terminal voltage under load: $V = \mathcal{E} - Ir$ , where $\mathcal{E}$ is the emf and $I$ is the current drawn.

The question asks whether this internal resistance stays constant and whether the electrolyte concentration remains unchanged during use. Both claims touch on what happens inside a cell as it discharges.

Examining the Assertion

Assertion (A): The internal resistance of a cell is constant.

This is false. Internal resistance depends on several factors:

Electrolyte concentration: As a cell discharges, chemical reactions consume the active materials. In a typical electrochemical cell, ions are converted or depleted, changing the ionic concentration of the electrolyte. Lower ion concentration means fewer charge carriers, which increases resistivity and thus internal resistance.

Temperature: Internal resistance decreases with rising temperature (ions move more freely) and increases when the cell cools.

Age and usage: Over time, electrode surfaces may become coated with reaction products (polarization), further increasing resistance.

State of charge: A nearly exhausted cell has significantly higher internal resistance than a fresh one.

In practice, $r$ increases noticeably as a cell is used, which is why old batteries deliver lower terminal voltages under the same load.

Examining the Reason

Reason (R): Ionic concentration of the electrolyte remains same during use of a cell.

This is also false. During discharge, electrochemical reactions at the electrodes consume reactants and produce products, directly altering the electrolyte composition.

For example, in a lead-acid cell:

At the anode: $\text{Pb} + \text{SO}_4^{2-} \to \text{PbSO}_4 + 2e^-$

At the cathode: $\text{PbO}_2 + 4\text{H}^+ + \text{SO}_4^{2-} + 2e^- \to \text{PbSO}_4 + 2\text{H}_2\text{O}$ …
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CBSE 2023Set ANNUAL1 mark
$Q. State the condition for maximum current to be drawn from a cell.$
›Reveal solutionSolution

Maximum current is drawn when the external resistance matches the internal resistance.

…

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CBSE 2022Set ANNUAL1 mark
$Q. What do you understand by internal resistance of a Cell?$
›Reveal solutionSolution

Internal resistance $r$ is the opposition to current flow offered by the cell's own electrolyte/electrodes.

Every real cell has some resistance to the flow of charge within itself, arising from the electrolyte and the electrode material -- this is called its internal resistance, denoted $r$ . Because of $r$ , when a cell of emf $\varepsilon$ drives a current $I$ through an external resistance $R$ , the terminal potential difference is $V = \varepsilon - Ir$ , which is less than the emf. Internal resistance depends on the nature of the electrolyte, the distance between the electrodes, the area of the electrodes, and the temperat …

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CBSE 2022Set ANNUAL1 mark
$Q. Under what condition, is terminal voltage of a cell equal to its Electromotive Force?$
›Reveal solutionSolution

Terminal voltage equals emf when the cell delivers no current, i.e. on open circuit.

For a cell of emf $\varepsilon$ and internal resistance $r$ supplying current $I$ , the terminal voltage is

$V = \varepsilon - I r.$

The drop $Ir$ across the internal resistance vanishes only when

$I = 0,$

so that $V = \varepsilon$ .

…

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Part (a)

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