Integrated Rate Equations

A rate law gives the instantaneous speed of a reaction, but a chemist watching a reactor rarely wants an instant — they want to know how much reactant survives after an hour, or a day. Integrated rate equations answer that practical question by turning the differential rate law into a direct formula linking concentration and time. For CBSE Class 12, only two cases are prescribed: zero order (rate stays constant, unaffected by how much reactant remains) and first order (rate falls in step with concentration). Each has its own concentration-time equation and its own half-life formula, and the two behave in opposite ways — one half-life grows as the reaction proceeds, the other stays fixed. Telling them apart from a graph, or from repeated half-life measurements, is a core exam skill this article builds.

The core insight

Integrating the differential rate law converts "how fast right now" into "how much is left after time t," giving [A]=[A]0−kt[A]=[A]_0-kt for zero order and k=2.303tlog⁡[A]0[A]k=\frac{2.303}{t}\log\frac{[A]_0}{[A]} for first order, with strikingly different half-life behaviour in each case.

The core idea

Why integrate at all. A rate law such as Rate=k[A]\text{Rate}=k[A] is a differential equation — it tells you the slope of the concentration-time curve at one moment, not the curve itself. Solving (integrating) that equation over time produces a formula you can actually plug numbers into: given a starting concentration and an elapsed time, predict what remains, or given two concentrations at two times, extract the rate constant kk.

Zero order case. Here the rate does not depend on concentration at all: Rate=k[A]0=k\text{Rate}=k[A]^0=k. Writing this as −d[A]dt=k-\dfrac{d[A]}{dt}=k and integrating from [A]0[A]_0 at t=0t=0 to [A][A] at time tt gives

[A]=[A]0−kt[A]=[A]_0-kt

where: [A]0[A]_0 is the initial concentration, [A][A] is the concentration remaining at time tt, and kk is the zero order rate constant (units mol L−1s−1\text{mol L}^{-1}\text{s}^{-1}). A plot of [A][A] against tt is a straight line of slope −k-k, so a zero order reaction is instantly recognisable graphically. Setting [A]=[A]0/2[A]=[A]_0/2 gives the half-life

t1/2=[A]02kt_{1/2}=\frac{[A]_0}{2k}

which grows as the starting concentration grows — a zero order reaction started more concentrated takes proportionally longer to reach its halfway point.

First order case. Here the rate is directly proportional to the one reactant's concentration: Rate=k[A]\text{Rate}=k[A]. Integrating −d[A]dt=k[A]-\dfrac{d[A]}{dt}=k[A] gives the natural-log form, more commonly used in its base-10 form:

ln⁡[A]0[A]=ktork=2.303tlog⁡[A]0[A]\ln\frac{[A]_0}{[A]}=kt \qquad\text{or}\qquad k=\frac{2.303}{t}\log\frac{[A]_0}{[A]}

where: the factor 2.303=ln⁡(10)2.303=\ln(10) converts log⁡10\log_{10} to ln⁡\ln, and kk here carries units s−1\text{s}^{-1} (no concentration unit, since it cancels in the ratio [A]0/[A][A]_0/[A]). A plot of log⁡[A]\log[A] against tt is linear with slope −k/2.303-k/2.303. The half-life comes out independent of starting concentration:

t1/2=0.693kt_{1/2}=\frac{0.693}{k}

This single difference — half-life depending on [A]0[A]_0 versus not — is the fastest experimental test for order: measure successive half-lives at different starting concentrations; if they come out equal, the reaction is first order.

Side by side. The two cases are easy to confuse under exam pressure, so it helps to hold them next to each other:

FeatureZero orderFirst order
Rate expressionRate=k\text{Rate}=kRate=k[A]\text{Rate}=k[A]
Integrated equation[A]=[A]0−kt[A]=[A]_0-ktk=2.303tlog⁡[A]0[A]k=\dfrac{2.303}{t}\log\dfrac{[A]_0}{[A]}
Units of kkmol L−1s−1\text{mol L}^{-1}\text{s}^{-1}s−1\text{s}^{-1}
Linear plot[A][A] vs. ttlog⁡[A]\log[A] vs. tt
t1/2t_{1/2} behaviourproportional to [A]0[A]_0independent of [A]0[A]_0

A quick way to remember why the units differ: in the zero order equation kk must have the same units as a concentration divided by time, since it is subtracted directly from [A]0[A]_0. In the first order equation, kk multiplies a bare logarithm (a pure ratio, no units), so kk carries only inverse time.

Figure
Concentration versus time curves for zero order and first order decay, with the zero order line straight and the first order curve bending toward the axis, each marked with its first two equal-fraction half-life intervals
Zero order versus first order decay of concentration with time time t concentration A zero order — straight line first order — curved decay half of A0
Derivation AThe first order integrated rate equation and half-life

Show, starting only from the differential rate law Rate=k[A]\text{Rate}=k[A] and using nothing beyond separation of variables and one definite integral, how the concentration-time formula k=2.303tlog⁡[A]0[A]k=\frac{2.303}{t}\log\frac{[A]_0}{[A]} and the half-life t1/2=0.693/kt_{1/2}=0.693/k both follow, and why the half-life comes out free of [A]0[A]_0.

Step 1. Write the rate law as a differential equation. Since AA is being consumed, Rate=−d[A]dt\text{Rate}=-\dfrac{d[A]}{dt}, and for a first order reaction Rate=k[A]\text{Rate}=k[A], so −d[A]dt=k[A]-\dfrac{d[A]}{dt}=k[A].

Step 2. Separate the variables so that every term with [A][A] sits on one side and every term with tt on the other: d[A][A]=−k dt\dfrac{d[A]}{[A]}=-k\,dt.

Step 3. Integrate both sides between the limits [A]0[A]_0 at t=0t=0 and [A][A] at time tt: ∫[A]0[A]d[A][A]=−k∫0tdt\displaystyle\int_{[A]_0}^{[A]}\frac{d[A]}{[A]}=-k\int_0^t dt, which gives ln⁡[A]−ln⁡[A]0=−kt\ln[A]-\ln[A]_0=-kt, or equivalently ln⁡[A]0[A]=kt\ln\dfrac{[A]_0}{[A]}=kt.

Step 4. Convert to base-10 logarithms, since ln⁡x=2.303log⁡x\ln x=2.303\log x, to reach the exam-standard form k=2.303tlog⁡[A]0[A]k=\dfrac{2.303}{t}\log\dfrac{[A]_0}{[A]}.

Step 5. Substitute [A]=[A]0/2[A]=[A]_0/2 to find the half-life: k=2.303t1/2log⁡[A]0[A]0/2=2.303t1/2log⁡2k=\dfrac{2.303}{t_{1/2}}\log\dfrac{[A]_0}{[A]_0/2}=\dfrac{2.303}{t_{1/2}}\log 2. Since log⁡2=0.301\log 2=0.301, this rearranges to t1/2=2.303×0.301k=0.693kt_{1/2}=\dfrac{2.303\times0.301}{k}=\dfrac{0.693}{k}. Because [A]0[A]_0 cancelled out at the substitution step, the half-life is independent of how much reactant you started with — the defining fingerprint of first order kinetics.

Worked example

The decomposition of N2O5N_2O_5 dissolved in CCl4CCl_4 is a standard first order CBSE example, with rate constant k=1.15×10−3 s−1k=1.15\times10^{-3}\ \text{s}^{-1} (the same value used for the pass-1 decomposition example). Suppose the initial concentration is [A]0=0.400 mol L−1[A]_0=0.400\ \text{mol L}^{-1}. Find (a) the concentration remaining after t=500 st=500\ \text{s}, and (b) confirm the half-life matches the 602.6 s602.6\ \text{s} value already known for this kk.

Step 1 — Set up the first order equation for the unknown concentration. log⁡[A]0[A]=kt2.303=(1.15×10−3)(500)2.303=0.5752.303=0.2497\log\dfrac{[A]_0}{[A]}=\dfrac{kt}{2.303}=\dfrac{(1.15\times10^{-3})(500)}{2.303}=\dfrac{0.575}{2.303}=0.2497.

Step 2 — Undo the logarithm. [A]0[A]=100.2497=1.778\dfrac{[A]_0}{[A]}=10^{0.2497}=1.778, so [A]=0.4001.778=0.225 mol L−1[A]=\dfrac{0.400}{1.778}=0.225\ \text{mol L}^{-1}.

Step 3 — Check against the half-life. t1/2=0.6931.15×10−3≈602.6 st_{1/2}=\dfrac{0.693}{1.15\times10^{-3}}\approx602.6\ \text{s}, matching the earlier value exactly, since t1/2t_{1/2} does not depend on [A]0=0.400[A]_0=0.400 any more than it depended on the earlier starting concentration.

Step 4 — Sanity check the answer. After 500 s500\ \text{s} (less than one half-life of 602.6 s602.6\ \text{s}), more than half the reactant should remain: 0.225/0.400=56.3%0.225/0.400=56.3\% remains, consistent with not quite reaching the halfway point. After 500 s, [A]≈0.225 mol L−1[A]\approx0.225\ \text{mol L}^{-1} remains, and the half-life is confirmed at 602.6 s regardless of the starting concentration used.

Competitive stretch

The same N2O5N_2O_5 reaction (k=1.15×10−3 s−1k=1.15\times10^{-3}\ \text{s}^{-1}) is monitored a second time, starting from [A]0=0.400 mol L−1[A]_0=0.400\ \text{mol L}^{-1} again. How many half-lives, and roughly how much time, does it take for the concentration to fall below 0.050 mol L−10.050\ \text{mol L}^{-1} — that is, to less than one-eighth of the starting amount?

Step 1 — Count half-lives needed. Each half-life halves the concentration: after 1 half-life, 0.2000.200 remains; after 2, 0.1000.100 remains; after 3, 0.0500.050 remains. So exactly 3 half-lives bring [A][A] from 0.4000.400 down to 0.050 mol L−10.050\ \text{mol L}^{-1}, since 0.400×(1/2)3=0.0500.400\times(1/2)^3=0.050.

Step 2 — Convert to time using the known half-life. With t1/2=602.6 st_{1/2}=602.6\ \text{s} from the previous example, 3 half-lives take 3×602.6=1808 s≈1810 s3\times602.6=1808\ \text{s}\approx1810\ \text{s}, or about 30 minutes.

Step 3 — Cross-check with the full logarithmic equation. t=2.303klog⁡0.4000.050=2.3031.15×10−3log⁡(8)=2002.6×0.903≈1808 st=\dfrac{2.303}{k}\log\dfrac{0.400}{0.050}=\dfrac{2.303}{1.15\times10^{-3}}\log(8)=2002.6\times0.903\approx1808\ \text{s}. Both routes agree: it takes 3 half-lives, about 1808 s (roughly 30 minutes), for the concentration to fall to one-eighth of its starting value — a useful shortcut whenever the target fraction is a power of one-half, since counting half-lives avoids the logarithm entirely.

Common traps

  • Using t1/2=0.693/kt_{1/2}=0.693/k for a zero order reaction or t1/2=[A]0/2kt_{1/2}=[A]_0/2k for a first order one — always confirm the order before picking a half-life formula; they are not interchangeable.
  • Dropping or misplacing the 2.3032.303 conversion factor when switching between ln⁡\ln and log⁡10\log_{10} in the first order equation.
  • Assuming half-life is a fixed property of every reaction — it is concentration-independent only for first order; for zero order it changes every time the starting concentration changes.
  • Reaching for a second-order integrated rate law on a CBSE problem — it has been removed from the current syllabus and should not appear in board-level answers.

Ask the tutor: Not sure whether a given data set is zero or first order, or want your half-life calculation checked — ask the AI tutor to walk through it with you.

How do I quickly tell zero order and first order apart from a data table without plotting anything

Compute successive half-lives from the data. Find the time to go from [A]0[A]_0 to [A]0/2[A]_0/2, then from [A]0/2[A]_0/2 to [A]0/4[A]_0/4. If those two intervals come out equal, the reaction is first order, since t1/2=0.693/kt_{1/2}=0.693/k never changes. If the second interval is noticeably shorter than the first, the reaction is zero order, since t1/2=[A]0/2kt_{1/2}=[A]_0/2k shrinks as the starting concentration for that stage shrinks.

Why does the first order equation use log base 10 with a 2.303 in it instead of just ln

The equation is naturally derived in natural logarithms, ln⁡([A]0/[A])=kt\ln([A]_0/[A])=kt, because that is what integration of 1/[A]1/[A] produces. CBSE problems traditionally give data as base-10 logarithms and use log tables, so the equation is rewritten using ln⁡x=2.303log⁡10x\ln x=2.303\log_{10}x, giving k=(2.303/t)log⁡([A]0/[A])k=(2.303/t)\log([A]_0/[A]). The 2.303 is not a new physical constant — it is purely the conversion factor between the two logarithm bases, and it must appear whenever you switch from ln⁡\ln to log⁡10\log_{10} in this equation.

If I am only given two data points, concentration at two different times, can I still find k without knowing the order

Not directly — you need to know (or assume) the order first, because the two orders use completely different equations. A common exam approach is to test both: compute kk assuming zero order using [A]=[A]0−kt[A]=[A]_0-kt, then compute kk assuming first order using the logarithmic equation, then check which assumption gives a constant kk across additional data points. Whichever order gives you the same kk value repeatedly, regardless of which two points you pick, is the correct order.

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Where this leads