According to the Arrhenius equation the rate constant is k = Ae-Ea/RT. Four possible straight-line plots of ln

NCERT Exemplar · Q6

k = A\,e^{-E_a/RT}

(i) a straight line starting from a high positive intercept on the

\ln k

axis and sloping DOWNWARD, so that

\ln k

decreases as

\tfrac{1}{T}

increases (negative slope);

(ii) a straight line sloping upward with a positive slope from a small positive intercept;

(iii) a straight line sloping upward with a positive slope from near the origin;

(iv) a straight line sloping upward with a gentle positive slope from a positive intercept. Which one correctly represents the graph of

\ln k

against

\tfrac{1}{T}

(i) Graph

(i) - a downward-sloping straight line (negative slope),

\ln k

decreasing as

\tfrac{1}{T}

increases.

(ii) Graph

(ii) - an upward-sloping straight line (positive slope) from a small positive intercept.

(iii) Graph

(iii) - an upward-sloping straight line (positive slope) from near the origin.

(iv) Graph

(iv) - an upward-sloping straight line (gentle positive slope) from a positive intercept.

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Concept understanding — Arrhenius Equation Plot

The Arrhenius Equation Plot: Why Temperature Changes Reaction Speed

You already know that heating things up makes reactions go faster. A cold chai takes forever to dissolve sugar; hot chai does it in seconds. But how much faster? And is there a pattern that holds for every reaction?

That pattern is the Arrhenius equation, and plotting it in a clever way reveals something fundamental about how molecules need to collide to react.

The core idea: an energy barrier

Imagine a ball sitting in a valley. To get to the next valley, it must first be pushed up over a hill. That hill is the activation energy ( $E_a$ ) — the minimum energy two molecules need to have when they collide, for the reaction to happen.

At a low temperature, most molecules move slowly. Only a tiny fraction have enough energy to climb that hill. Raise the temperature, and suddenly many more molecules have the required energy. The fraction of molecules with energy $\ge E_a$ is given by the Boltzmann distribution:

\text{fraction} = e^{-E_a / RT}

where $R$ is the gas constant and $T$ is the absolute temperature (in Kelvin). This exponential is the heart of the story.

The Arrhenius equation (precise statement)

The rate constant $k$ of a reaction depends on temperature as:

k = A \, e^{-E_a / RT}

$k$ = rate constant (how fast the reaction proceeds)
$A$ = pre-exponential factor (frequency of collisions, times a steric factor — how often molecules hit in the right orientation)
$E_a$ = activation energy (J/mol or kJ/mol)
$R$ = 8.314 J/(mol·K)
$T$ = temperature in Kelvin

Important

$k$ is not the reaction rate itself — it's the proportionality constant in the rate law. But for a fixed concentration, a larger $k$ means a faster reaction.

Why plot it? The linear trick

The equation $k = A e^{-E_a / RT}$ is exponential in $1/T$ . That's hard to eyeball. But take the natural logarithm of both sides:

\ln k = \ln A - \frac{E_a}{R} \cdot \frac{1}{T}

This is the equation of a straight line:

y = c + m x

where:

$y = \ln k$
$x = 1/T$
slope $m = -E_a / R$
intercept $c = \ln A$

So if you measure $k$ at several temperatures and plot $\ln k$ versus $1/T$ , you get a straight line — provided the reaction follows Arrhenius behaviour (most do, over moderate temperature ranges).

Tip

Always use Kelvin for $T$ . Celsius will give you a curved mess because $1/T$ is not linear in Celsius.

What the plot tells you

From the slope, you get $E_a$ :

E_a = - (\text{slope}) \times R

A steep negative slope means a large $E_a$ — the reaction is very sensitive to temperature. A shallow slope means a small $E_a$ — temperature doesn't affect it much.

From the intercept, you get $A$ :

A = e^{\text{intercept}}

This tells you about the collision frequency and orientation factor. A high $A$ means molecules are colliding often and in the right geometry.

A typical Arrhenius plot looks like this

$T$ (K)	$k$ (s⁻¹)	$1/T$ (K⁻¹)	$\ln k$
300	0.0012	0.00333	-6.72
310	0.0028	0.00323	-5.88
320	0.0061	0.00313	-5.10
330	0.0125	0.00303	-4.38

Plot $\ln k$ (y-axis) vs $1/T$ (x-axis). The points fall on a straight line. Draw the best-fit line, measure its slope, and compute $E_a$ . …

Why this formula?

Arrhenius Equation Plot: Why It Holds

The Arrhenius equation is not a guess — it emerges from a deep physical picture of how molecules react. Let's build that understanding step by step.

The Core Idea: Molecules Need Energy to React

For a reaction to occur, molecules must collide with enough energy to break existing bonds and form new ones. This minimum energy is called the activation energy ( $E_a$ ).

But not all collisions succeed — only those with kinetic energy $\geq E_a$ lead to a reaction.

The Key Formula

The Arrhenius equation is:

k = A e^{-E_a / (RT)}

Where:

$k$ = rate constant
$A$ = pre-exponential factor (frequency of collisions with correct orientation)
$E_a$ = activation energy (J/mol)
$R$ = gas constant (8.314 J/mol·K)
$T$ = absolute temperature (K)

Why the Exponential Term Appears

Step 1: The Boltzmann Distribution

Molecules in a gas or liquid have a distribution of kinetic energies. The fraction of molecules with energy $\geq E$ is given by the Boltzmann factor:

\text{Fraction} = e^{-E / (k_B T)}

For molar quantities, replace $k_B$ with $R$ :

\text{Fraction} = e^{-E_a / (RT)}

This is not arbitrary — it comes from statistical mechanics. The exponential arises because the probability of a molecule having energy $E$ decreases exponentially as $E$ increases.

Step 2: Rate Depends on This Fraction

The rate constant $k$ is proportional to:

The collision frequency (how often molecules meet)
The fraction of collisions with energy $\geq E_a$

Thus:

k \propto \text{(collision frequency)} \times e^{-E_a / (RT)}

The collision frequency is captured by $A$ , giving:

k = A e^{-E_a / (RT)}

Why the Plot is Linear

Take the natural logarithm of both sides:

\ln k = \ln A - \frac{E_a}{R} \cdot \frac{1}{T}

This is of the form $y = mx + c$ , where:

$y = \ln k$
$x = 1/T$
Slope $m = -E_a / R$
Intercept $c = \ln A$

Thus, plotting $\ln k$ vs $1/T$ gives a straight line — this is the Arrhenius plot.

What the Slope Tells Us

From the slope: …

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Taking logarithms of $k=A\,e^{-E_a/RT}$ gives $\ln k=\ln A-\frac{E_a}{R}\cdot\frac{1}{T}$ - a straight line in $\ln k$ versus $\frac{1}{T}$ with negative slope $-\frac{E_a}{R}$ and intercept $\ln A$ . Only graph (i) has a negative slope.

Concept

The linearised Arrhenius equation has the form $y=c+mx$ with $y=\ln k$ , $x=\frac{1}{T}$ , slope $m=-\frac{E_a}{R}$ and intercept $c=\ln A$ .

Working

$\ln k=\ln A-\frac{E_a}{R}\,\frac{1}{T}$ …

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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 25 on this concept.

TG EAPCET 2026Set ap-2026-05-04-AN1 markMCQ
$^+$
›Reveal solutionSolution
For a hydrogen-like ion, the radius and energy of an orbit are linked through the Bohr model. Using the given radius of He⁺, we find the principal quantum number $n$ , then compute the energy. The energy of that orbit is $-9.68 \times 10^{-22}$ kJ.

The key idea here is that for any hydrogen-like species (one electron around a nucleus of charge $Ze$ ), the Bohr model gives exact expressions for both the radius and the energy of the $n$ th orbit. The radius depends on $n^2/Z$ , and the energy depends on $Z^2/n^2$ . If you know one, you can find the other.

The problem gives the radius of an orbit of He⁺ ( $Z=2$ ) as 238.05 pm. That number is not arbitrary — it should match a specific $n$ value. Once $n$ is known, the energy follows directly. Let’s work through it.

Recall the Bohr radius formula for a hydrogen-like ion. The radius of the $n$ th orbit is

$r_n = \frac{n^2}{Z} a_0$
where $a_0 = 52.9$ pm is the Bohr radius (the radius of the first orbit in hydrogen). For He⁺, $Z=2$ , so
$r_n = \frac{n^2}{2} \times 52.9 \text{ pm}$

Plug in the given radius and solve for $n$ . We have $r_n = 238.05$ pm. Thus

$238.05 = \frac{n^2}{2} \times 52.9$
Multiply both sides by 2:
$476.1 = n^2 \times 52.9$
Divide by 52.9:
$n^2 = \frac{476.1}{52.9} = 9$
So $n = 3$ . The orbit is the third Bohr orbit of He⁺.

Tip

You could also notice that 238.05 pm is exactly $4.5 \times 52.9$ pm, and $4.5 = 9/2$ , so $n^2 = 9$ immediately. Spotting such ratios saves time in exams.

Now find the energy of the $n$ th orbit for He⁺. The energy of a hydrogen-like ion in the $n$ th orbit is

$E_n = -13.6 \times \frac{Z^2}{n^2} \text{ eV}$
For He⁺ ( $Z=2$ ) and $n=3$ :
$E_3 = -13.6 \times \frac{4}{9} \text{ eV} = -13.6 \times \frac{4}{9} \text{ eV}$
Compute:

$-13.6 \times \frac{4}{9} = -\frac{54.4}{9} = -6.0444\ldots \text{ eV}$ …
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TG EAPCET 2026Set ap-2026-05-05-FN1 markMCQ
$\begin{array}{|c|c|} \hline \text{Time(s)} & \text{Total pressure (in atm)} \\ \hline 0 & 0.5 \\ 100 & 0.6 \\ \hline \end{array}$
›Reveal solutionSolution
For a first-order gas-phase decomposition, the total pressure increases as the reactant decomposes. Using the relation between total pressure and partial pressure of the reactant, we apply the first-order integrated rate law to find $k = 2.23 \times 10^{-3} \, \text{s}^{-1}$ .

The key idea here is that the total pressure in a constant-volume system is not the same as the concentration of the reactant — but for a gas-phase reaction, partial pressure is directly proportional to concentration. So we can track the reaction by converting the measured total pressure into the partial pressure of A at any time.

The reaction is:

$A(g) \rightarrow \text{products}$ (assume stoichiometry like $A \rightarrow B + C$ or similar, typical for first-order decomposition where moles increase).

Let’s work through it step by step.

Write the reaction and initial conditions.

Suppose $A(g)$ decomposes as $A(g) \rightarrow B(g) + C(g)$ (or any number of product gases). At $t=0$ , only A is present, so initial pressure $P_A(0) = 0.5$ atm. Total pressure at $t=0$ is also $0.5$ atm.

Relate total pressure to partial pressure of A.

Let the initial pressure of A be $P_0 = 0.5$ atm. At time $t$ , let $x$ be the amount (in atm) of A that has decomposed. Then:

Partial pressure of A remaining: $P_A = P_0 - x$

If the reaction produces, say, 1 mole of B and 1 mole of C per mole of A, then partial pressures of products are $x$ each.

Total pressure: $P_{\text{total}} = (P_0 - x) + x + x = P_0 + x$

So $x = P_{\text{total}} - P_0$ .

Find $P_A$ at $t = 100$ s.

Given $P_{\text{total}} = 0.6$ atm at $t=100$ s, we have:

$x = 0.6 - 0.5 = 0.1 \text{ atm}$
Therefore:
$P_A(100) = P_0 - x = 0.5 - 0.1 = 0.4 \text{ atm}$

Apply the first-order rate law. For a first-order reaction, the integrated rate law in terms of pressure (since $P \propto$ concentration at constant $T$ and $V$ ) is:

$k = \frac{1}{t} \ln \frac{P_0}{P_A}$
Substitute $t = 100$ s, $P_0 = 0.5$ , $P_A = 0.4$ :
$k = \frac{1}{100} \ln \frac{0.5}{0.4} = \frac{1}{100} \ln(1.25)$

Use the given log value. …
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TG EAPCET 2025Set eng-2025-05-02-FN1 markMCQ
$\ce{R -> P}$
›Reveal solutionSolution

A half-life independent of initial concentration identifies a first-order reaction, for which $[R]$ falls exponentially with time. So the plot showing $[R]$ itself as a straight line is the incorrect one — option (B).

The concept first

Start from the rate law and integrate.

First order: $-\dfrac{d[R]}{dt}=k[R]$ gives
$\ln\frac{[R]_0}{[R]}=kt\qquad\Longleftrightarrow\qquad \ln[R]=\ln[R]_0-kt,$
and hence the half-life
$t_{1/2}=\frac{\ln 2}{k}=\frac{0.693}{k},$
which contains no $[R]_0$ — exactly the property stated in the question. (For a zero-order reaction $t_{1/2}=[R]_0/2k$ , and for second order $t_{1/2}=1/k[R]_0$ ; both do depend on $[R]_0$ .) So the reaction is first order.

The important structural consequence: in first-order kinetics it is the logarithm of the concentration that falls linearly, not the concentration itself.

Step 1 — Check graph (A): $\ln[R]$ vs $t$
$\ln[R]=\ln[R]_0-kt$
Straight line, intercept $\ln[R]_0$ , slope $-k$ , so $k=-\text{slope}$ . Correct.

Step 2 — Check graph (C): $\log[R]$ vs $t$

Divide the same equation by $2.303$ :
$\log[R]=\log[R]_0-\frac{k}{2.303}\,t$
Slope $=-\dfrac{k}{2.303}$ , so $k=-\text{slope}\times 2.303$ . Correct. …
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TG EAPCET 2025Set eng-2025-05-04-FN1 markMCQ
$4.242$
›Reveal solutionSolution
In a face-centered cubic (fcc) lattice, atoms touch along the face diagonal, leading to the relationship $4r = \sqrt{2}a$ , where $r$ is the atomic radius and $a$ is the edge length. For an edge length of $4.242$ Å, the radius of the M atom is $\boxed{1.5}$ Å.

Concept and Intuition

When a metal crystallizes in a face-centered cubic (fcc) lattice, it means the atoms are located at all eight corners of the cube and at the center of each of the six faces. To understand the relationship between the edge length ( $a$ ) of the unit cell and the radius ( $r$ ) of the atom, we need to identify where the atoms are in direct contact.

In an fcc structure, the atoms at the corners do not touch each other along the edge of the cube. Instead, the atoms touch along the face diagonal. Imagine one face of the cube: there are atoms at the two opposite corners of that face, and a third atom exactly in the center of that face. These three atoms are in contact along the face diagonal.

Consider a face of the cube with edge length $a$ . The length of the face diagonal can be found using the Pythagorean theorem. If we consider a right-angled triangle formed by two edges and the face diagonal, the diagonal is the hypotenuse.

Let the edge length be $a$ .

The face diagonal, $d$ , is given by:

$d^2 = a^2 + a^2$

$d^2 = 2a^2$

$d = \sqrt{2}a$

Along this face diagonal, we have a corner atom (radius $r$ ), followed by the face-centered atom (diameter $2r$ ), and then another corner atom (radius $r$ ). Therefore, the total length of the face diagonal is $r + 2r + r = 4r$ .

Equating these two expressions for the face diagonal:

$4r = \sqrt{2}a$

This is the fundamental relationship for an fcc lattice that allows us to calculate the atomic radius if the edge length is known, or vice versa.
$r$
Step-by-step Solution

Identify the given information:

We are given that the metal M crystallizes in an fcc lattice and its edge length ( $a$ ) is $4.242$ Å.

Recall the relationship between edge length and atomic radius for an fcc lattice:

As derived above, for an fcc lattice, the atoms touch along the face diagonal. The length of the face diagonal is $\sqrt{2}a$ , and it is also equal to $4r$ (where $r$ is the atomic radius).

So, we have the formula: …
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TG EAPCET 2025Set ap-2025-04-29-AN1 markMCQ
$0.082\ \mathrm{L\,K^{-1}}$
›Reveal solutionSolution
The slope of an isobar (constant pressure) on a $V$ – $T$ graph for one mole of an ideal gas is $\frac{R}{p}$ . Equating this to the given slope $0.082\ \mathrm{L\,K^{-1}}$ and using $R = 0.082\ \mathrm{L\,atm\,mol^{-1}\,K^{-1}}$ gives $p = 1\ \mathrm{atm}$ .

The key here is to connect the physical meaning of an isobar to the ideal gas law. An isobar is a line of constant pressure on a graph — typically volume $V$ against temperature $T$ . For one mole of an ideal gas, the equation of state is $pV = RT$ . When $p$ is fixed, $V$ and $T$ are directly proportional: $V = \left(\frac{R}{p}\right) T$ . This is a straight line through the origin, and its slope is $\frac{R}{p}$ .

The problem gives you that slope numerically: $0.082\ \mathrm{L\,K^{-1}}$ . You also know $R = 0.082\ \mathrm{L\,atm\,mol^{-1}\,K^{-1}}$ . So you can set up a simple equation.

Write the ideal gas law for one mole: $pV = RT$ .

At constant $p$ , rearrange to $V = \frac{R}{p} T$ .

This is of the form $V = (\text{slope}) \times T$ , so the slope of the isobar on a $V$ – $T$ graph is $\frac{R}{p}$ .

The given slope is $0.082\ \mathrm{L\,K^{-1}}$ . Therefore:

$\frac{R}{p} = 0.082\ \mathrm{L\,K^{-1}}$

Substitute $R = 0.082\ \mathrm{L\,atm\,mol^{-1}\,K^{-1}}$ :

$\frac{0.082}{p} = 0.082$

Solve for $p$ : Multiply both sides by $p$ : $0.082 = 0.082\,p$ …
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TG EAPCET 2025Set ap-2025-04-29-FN1 markMCQ
$m_A$
›Reveal solutionSolution
For a first-order reaction, the rate (and hence the slope of a concentration vs. time plot) is proportional to the instantaneous concentration. As concentration decreases from A to B to C, the slope becomes less negative. The correct order is $m_A > m_B > m_C$ .

The graph shows concentration of reactant A versus time for a first-order reaction. The slope at any point on this curve represents the rate of change of concentration with time, which is precisely the reaction rate (with a negative sign, since concentration decreases).

For a first-order reaction, the rate law is:
$-\frac{d[A]}{dt} = k[A]$
This tells us that the rate at any instant is directly proportional to the concentration at that instant. Higher concentration means faster reaction, which means a steeper (more negative) slope on the concentration-time graph.

Now let's trace what happens as we move from point A to B to C along the curve:

At point A (earliest time): The concentration is highest. The reaction proceeds most rapidly here, so $\frac{d[A]}{dt}$ is most negative. The slope $m_A$ has the largest magnitude in the negative direction.

At point B (intermediate time): Concentration has decreased compared to A. The reaction rate has slowed down, so $\frac{d[A]}{dt}$ is less negative than at A. The slope $m_B$ has a smaller magnitude.

At point C (latest time): Concentration is lowest among the three points. The reaction is slowest here, so $\frac{d[A]}{dt}$ is least negative. The slope $m_C$ has the smallest magnitude. …
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TG EAPCET 2025Set ap-2025-04-30-FN1 markMCQ
$0.82\, \text{L K}^{-1}$
›Reveal solutionSolution
The slope of an isobar on a $V$ – $T$ graph for one mole of an ideal gas is $\frac{nR}{P}$ . Equating this to $0.82\ \text{L K}^{-1}$ and using $R = 0.0821\ \text{L atm mol}^{-1}\text{K}^{-1}$ gives $P = 0.1\ \text{atm}$ .

The key is to recognise what an isobar means physically: a process at constant pressure. For an ideal gas, the relation between volume and temperature at fixed pressure is given by the ideal gas law. The slope of the $V$ – $T$ graph at constant $P$ is not just any number — it is directly linked to $nR/P$ .

Let’s unpack that.

Start with the ideal gas law For one mole of an ideal gas:

$PV = nRT \quad \Rightarrow \quad PV = RT \quad (\text{since } n=1)$
At constant pressure $P$ , this becomes a linear relation between $V$ and $T$ :
$V = \frac{R}{P}\, T$
So $V$ is directly proportional to $T$ , and the graph of $V$ vs $T$ is a straight line through the origin.

Identify the slope The slope of this line is the coefficient of $T$ :

$\text{slope} = \frac{R}{P}$
The problem gives this slope as $0.82\ \text{L K}^{-1}$ .

Use the correct value of $R$ Since the slope is in $\text{L K}^{-1}$ and pressure is in atm, we must use $R$ in compatible units:

$R = 0.0821\ \text{L atm mol}^{-1}\text{K}^{-1}$
This is a standard value you must remember for such problems.

Set up and solve $\frac{R}{P} = 0.82 \quad \Rightarrow \quad P = \frac{R}{0.82}$ …
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TG EAPCET 2025Set ap-2025-04-30-FN1 markMCQ
$\rightarrow$
›Reveal solutionSolution

For a first-order reaction, the integrated rate law gives $\ln \frac{[\text{R}]_0}{[\text{R}]} = kt$ , so a plot of $\ln \frac{[\text{R}]_0}{[\text{R}]}$ vs. time is a straight line through the origin with slope $k$ . Hence the slope $x$ equals the rate constant $k$ , and the answer is (C).

The key here is to recall the integrated rate law for a first-order reaction. For a reaction $\text{R} \rightarrow \text{P}$ , the rate depends on the concentration of R as:
$-\frac{d[\text{R}]}{dt} = k[\text{R}]$
Integrating this from initial concentration $[\text{R}]_0$ at $t=0$ to $[\text{R}]$ at time $t$ gives:
$\ln \frac{[\text{R}]_0}{[\text{R}]} = kt$
This is the straight-line form: if you plot $\ln \frac{[\text{R}]_0}{[\text{R}]}$ on the $y$ -axis and time $t$ on the $x$ -axis, you get a line with slope $k$ and intercept $0$ (passing through the origin). No conversion factor like $2.303$ appears because we are using natural logarithms, not base-10 logs. …
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TG EAPCET 2024Set ap-2024-05-08-FN1 markMCQ
$\rightarrow$
›Reveal solutionSolution
Integrating the first-order rate law gives $\log\dfrac{a}{a-x} = \dfrac{k}{2.303}t$ — a straight line through the origin with positive slope. That is exactly the graph in option (D).

The concept first: deriving the first-order integrated rate law

Let the initial concentration of $A$ be $a$ and let $x$ be the amount that has reacted after time $t$ , so the concentration remaining is $(a-x)$ .

Step 1 — write the differential rate law. For a first-order reaction the rate is proportional to the first power of the reactant concentration:
$\text{rate} = \frac{\mathrm{d}x}{\mathrm{d}t} = k\,(a-x)$
Step 2 — separate the variables.
$\frac{\mathrm{d}x}{a-x} = k\,\mathrm{d}t$
Step 3 — integrate between the limits $x=0$ at $t=0$ and $x=x$ at $t=t$ .
$\int_0^x \frac{\mathrm{d}x}{a-x} = k\int_0^t \mathrm{d}t \quad\Longrightarrow\quad -\ln(a-x)\Big|_0^x = kt$ $\ln\frac{a}{a-x} = kt \quad\Longrightarrow\quad \boxed{k = \frac{2.303}{t}\log\frac{a}{a-x}}$
Step 4 — put it into straight-line form $y = mx + c$ .
$\log\frac{a}{a-x} \;=\; \underbrace{\frac{k}{2.303}}_{\text{slope } m}\; t \;+\; \underbrace{0}_{\text{intercept}}$
Read off the three things a graph question always wants:

$y$ -variable: $\log\dfrac{a}{a-x}$

slope: $+\dfrac{k}{2.303}$ — positive (since $k>0$ )

intercept: zero — the line passes through the origin. This is physically obvious: at $t=0$ nothing has reacted, $x=0$ , so $\log\frac{a}{a}= \log 1 = 0$ .

Step 5 — test the printed options

(A) plots $a$ (a constant, the initial concentration) against $t$ . A constant cannot rise with a positive slope; meaningless. ✗ …
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TG EAPCET 2024Set eng-2024-05-09-FN1 markMCQ
$\dfrac{9}{8R}$
›Reveal solutionSolution
The Balmer series corresponds to transitions ending at $n=2$ ; the wavelength is given by $\frac{1}{\lambda}=R\left(\frac{1}{2^2}-\frac{1}{n^2}\right)$ . Evaluating the four options shows that only $\frac{100}{21R}$ matches a valid Balmer transition ( $n=5\to2$ ), so the correct option is (B).

The Balmer series of the hydrogen atom consists of spectral lines produced when an electron falls from a higher energy level ( $n \ge 3$ ) to the second energy level ( $n=2$ ). The Rydberg formula for the wavelength $\lambda$ of such a transition is:
$\frac{1}{\lambda} = R \left( \frac{1}{2^2} - \frac{1}{n^2} \right), \quad n = 3,4,5,\dots$
where $R$ is the Rydberg constant. Our task is to see which of the given expressions for $\lambda$ (in terms of $R$ ) can be written in the form $\frac{1}{\lambda} = R \cdot (\text{some rational number})$ that matches a valid $n$ .

Rewrite each option as $1/\lambda$ For an option $\lambda = \frac{a}{bR}$ , we have

$\frac{1}{\lambda} = \frac{bR}{a}.$
This must equal $R\left(\frac{1}{4} - \frac{1}{n^2}\right)$ for some integer $n \ge 3$ .

Test option (A): $\lambda = \frac{9}{8R}$

$\frac{1}{\lambda} = \frac{8R}{9} = R \cdot \frac{8}{9}.$
Set $\frac{1}{4} - \frac{1}{n^2} = \frac{8}{9}$ . Then $\frac{1}{n^2} = \frac{1}{4} - \frac{8}{9} = \frac{9-32}{36} = -\frac{23}{36}$ , which is negative — impossible. So (A) is invalid.

Test option (B): $\lambda = \frac{100}{21R}$

$\frac{1}{\lambda} = \frac{21R}{100} = R \cdot \frac{21}{100}.$
Solve $\frac{1}{4} - \frac{1}{n^2} = \frac{21}{100}$ .
$\frac{1}{n^2} = \frac{1}{4} - \frac{21}{100} = \frac{25}{100} - \frac{21}{100} = \frac{4}{100} = \frac{1}{25}.$
Hence $n^2 = 25$ and $n = 5$ . Since $n=5$ is a valid upper level ( $n \ge 3$ ), this works. So (B) corresponds to the $5\to2$ transition.

Test option (C): $\lambda = \frac{25}{24R}$

$\frac{1}{\lambda} = \frac{24R}{25} = R \cdot \frac{24}{25}.$
Then $\frac{1}{4} - \frac{1}{n^2} = \frac{24}{25}$ gives $\frac{1}{n^2} = \frac{1}{4} - \frac{24}{25} = \frac{25-96}{100} = -\frac{71}{100}$ — negative. Invalid. …
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TG EAPCET 2024Set eng-2024-05-09-FN1 markMCQ
$\frac{x}{m}$
›Reveal solutionSolution
The Freundlich isotherm is $\log(x/m) = \log k + (1/n)\log P$ ; given slope $1/n = 0.5$ and intercept $\log k = 1.0$ , at $P = 100$ we get $\log(x/m) = 1.0 + 0.5 \times 2 = 2.0$ , so $x/m = 100$ . The correct option is (C).

Concept & Intuition

The Freundlich adsorption isotherm describes how the amount of gas adsorbed per unit mass of adsorbent ( $x/m$ ) varies with pressure $P$ . It is an empirical relation:
$\frac{x}{m} = k P^{1/n}$
where $k$ and $n$ are constants. Taking logarithms gives a straight line:
$\log\left(\frac{x}{m}\right) = \log k + \frac{1}{n} \log P$
Here, the slope is $1/n$ and the intercept (on the $\log(x/m)$ axis) is $\log k$ . The problem gives slope = 0.5 and intercept = 1.0 — but careful: these are the slope and intercept of the log–log plot, not of the original curve. So we directly plug into the linear form.

Step-by-step

Write the linear form of the Freundlich isotherm

$\log\left(\frac{x}{m}\right) = \log k + \frac{1}{n} \log P$
The slope is $1/n = 0.5$ , and the intercept (y-intercept) is $\log k = 1.0$ .

Substitute the given pressure Pressure $P = 100$ atm. Compute $\log P$ (using base 10, as is standard for such plots):

$\log_{10}(100) = 2$

Calculate $\log(x/m)$

$\log\left(\frac{x}{m}\right) = 1.0 + 0.5 \times 2 = 1.0 + 1.0 = 2.0$

Find $x/m$ …
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TG EAPCET 2024Set eng-2024-05-10-AN1 markMCQ
$\log \dfrac{a}{(a-x)}$
›Reveal solutionSolution
For a first‑order reaction, the integrated rate law gives $\log\frac{a}{a-x} = \frac{k}{2.303}\,t$ , so the slope of the $\log\frac{a}{a-x}$ vs. $t$ plot is $k/2.303$ . With slope $2\times10^{-3}$ min $^{-1}$ , the rate constant is $k = 2.303 \times 2\times10^{-3} = 4.606\times10^{-3}$ min $^{-1}$ , which corresponds to option (C).

Concept & Intuition

For a first‑order reaction $\mathrm{A \to products}$ , the concentration of reactant at time $t$ is given by
$\ln\frac{a}{a-x} = kt$
where $a$ is the initial concentration and $x$ is the amount reacted.

If we convert natural log to base‑10 log, we get
$\log\frac{a}{a-x} = \frac{k}{2.303}\,t.$
This is a straight line through the origin when $\log\frac{a}{a-x}$ is plotted against $t$ . The slope of that line is not $k$ itself, but $k/2.303$ . Many students mistakenly take the slope directly as the rate constant — that’s the classic pitfall here.

Step‑by‑step reasoning

Write the first‑order integrated rate law in base‑10 form

$\log\frac{a}{a-x} = \frac{k}{2.303}\,t$
This is of the form $y = m\,t$ , where $y = \log\frac{a}{a-x}$ and $m$ is the slope.

Identify the given slope The problem states the slope of the straight line is $2 \times 10^{-3}$ min $^{-1}$ . So

$\text{slope} = \frac{k}{2.303} = 2 \times 10^{-3}$

Solve for the rate constant $k$ …
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Q.According to the Arrhenius equation the rate constant is k=A e−Ea/RTk = A\,e^{-E_a/RT}k=Ae−Ea​/RT. Four possible straight-line plots of ln⁡k\ln klnk (vertical axis) against 1T\tfrac{1}{T}T1​ (horizontal axis) are proposed:

Concept

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Q.According to the Arrhenius equation the rate constant is $k = A\,e^{-E_a/RT}$ . Four possible straight-line plots of $\ln k$ (vertical axis) against $\tfrac{1}{T}$ (horizontal axis) are proposed:

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