IMO Practice Test — Atoms and Nuclei
14 Questions • 15 min • Olympiad level
15:00
Question 1 of 14
The ratio of the radii of the third and first Bohr orbits of hydrogen is:
$3 : 1$
$9 : 1$
$1 : 9$
$1 : 3$
Explanation: $r_n \propto n^2$, so $r_3 : r_1 = 9 : 1$.
Question 2 of 14
The ratio of the longest wavelength of the Lyman series to that of the Balmer series is:
$5 : 27$
$27 : 5$
$1 : 3$
$3 : 1$
Explanation: Lyman ($2\to1$): $1/\lambda = R(3/4)$. Balmer ($3\to2$): $1/\lambda = R(5/36)$. Ratio of wavelengths $= \frac{4/3}{36/5} = \frac{20}{108} = \frac{5}{27}$.
Question 3 of 14
The shortest wavelength (series limit) of the Lyman series corresponds to a transition from:
$n = 2 \to 1$
$n = 3 \to 1$
$n = \infty \to 1$
$n = \infty \to 2$
Explanation: The series limit is the $n = \infty \to 1$ transition, giving the shortest $\lambda$.
Question 4 of 14
If the radius of a nucleus of mass number 27 is $3.6\ \text{fm}$, the radius of a nucleus of mass number 64 is:
$2.7\ \text{fm}$
$5.4\ \text{fm}$
$7.2\ \text{fm}$
$4.8\ \text{fm}$
Explanation: $R \propto A^{1/3}$: $R = 3.6 \times (64/27)^{1/3} = 3.6 \times \frac{4}{3} = 4.8\ \text{fm}$.
Question 5 of 14
A nucleus emits one $\alpha$ and two $\beta^-$ particles. Compared with the parent, the daughter has:
the same atomic number
atomic number lower by 2
atomic number higher by 1
mass number lower by 2
Explanation: $Z$: $-2$ (from $\alpha$) $+2$ (from two $\beta^-$) $= 0$ net; $A$ falls by 4. Same $Z$ means it is an isotope of the parent.
Question 6 of 14
A sample decays to $\frac{1}{16}$ of its initial value in 8 hours. Its half-life is:
1 hour
4 hours
2 hours
8 hours
Explanation: $\frac{1}{16} = (1/2)^4$, so 4 half-lives in 8 hr means $T_{1/2} = 2\ \text{hr}$.
Question 7 of 14
Two radioactive samples have half-lives in the ratio $1 : 2$ and the same number of initial nuclei. After a time equal to two half-lives of the first, the ratio of remaining nuclei (first : second) is:
$1 : 1$
$2 : 1$
$1 : 4$
$1 : 2$
Explanation: In time $2T$ (with $T_2 = 2T$): first undergoes 2 half-lives ($1/4$), second undergoes 1 half-life ($1/2$). Ratio $= (1/4):(1/2) = 1 : 2$.
Question 8 of 14
The binding energy of a deuteron ${}^{2}_{1}\text{H}$ is $2.2\ \text{MeV}$. Its binding energy per nucleon is:
$2.2\ \text{MeV}$
$1.1\ \text{MeV}$
$4.4\ \text{MeV}$
$0.55\ \text{MeV}$
Explanation: $\frac{E_b}{A} = \frac{2.2}{2} = 1.1\ \text{MeV per nucleon}$.
Question 9 of 14
When a hydrogen atom is excited from $n=1$ to $n=4$, the number of distinct spectral lines that can be emitted is:
6
4
3
10
Explanation: Number of lines $= \frac{n(n-1)}{2} = \frac{4 \times 3}{2} = 6$.
Question 10 of 14
If $1\ \text{u}$ of mass is fully converted to energy, the energy obtained is closest to:
$931.5\ \text{keV}$
$93.15\ \text{MeV}$
$931.5\ \text{MeV}$
$9.315\ \text{MeV}$
Explanation: $1\ \text{u} \equiv 931.5\ \text{MeV}$ by $E = mc^2$.
Question 11 of 14
The activity of a radioactive sample falls from $8000\ \text{Bq}$ to $1000\ \text{Bq}$ in 9 days. The half-life is:
1 day
9 days
4.5 days
3 days
Explanation: $\frac{1000}{8000} = \frac{1}{8} = (1/2)^3$, so 3 half-lives in 9 days $\Rightarrow T_{1/2} = 3\ \text{days}$.
Question 12 of 14
In the fusion reaction $4\,{}^{1}_{1}\text{H} \to {}^{4}_{2}\text{He} + 2e^{+} + \text{energy}$, the energy comes from:
the kinetic energy of protons only
the increase in binding energy per nucleon
the charge of the positrons
the gravitational field of the Sun
Explanation: Helium has a higher binding energy per nucleon than hydrogen, so the surplus is released as energy ($\Delta m\, c^2$).
Question 13 of 14
The wavelength of the $\text{H}_\alpha$ line ($n=3 \to 2$) is $656\ \text{nm}$. The energy of this photon is about:
$3.4\ \text{eV}$
$13.6\ \text{eV}$
$1.89\ \text{eV}$
$12.1\ \text{eV}$
Explanation: $E = \frac{1240}{656} \approx 1.89\ \text{eV}$, matching $E_3 - E_2$.
Question 14 of 14
A heavy nucleus splits into two equal fragments. Compared with the parent, the radius of each fragment is:
$\frac{1}{2^{1/3}}$ times the parent radius
half the parent radius
the same
twice the parent radius
Explanation: Each fragment has $A/2$, and $R \propto A^{1/3}$, so $R_f = R_p (1/2)^{1/3} = \frac{R_p}{2^{1/3}}$.