With the old Quanta to Quarks elective being examined for the last time this November a list of true-false questions on concepts that are often misunderstood is given below. This list will be updated during the next six weeks.
Rutherford Model of the Atom
- Rutherford's model of the atom has a central charge concentration made of protons and neutrons.
- The alpha particles that bounce back from the gold foil hit the nuclei of the atoms in the foil.
- Rutherford's model did not have electrons orbiting the nucleus in rings
- In Rutherford scattering the number of alpha partices scattered through 60 degrees is one-half the number scattered through 30 degrees.
- If the thickness of the gold foil is doubled the number of alpha particles scattered through each angle is halved.
- In the Geiger and Marsden 1910 scattering experiment the number of alpha particles scattered through an angle greater than 90 degrees was 1 in 800.
- Alpha particles released in the decay of Ra-226 have different kinetic energies.
- Beta particles given off in the decay of Sr-90 have the same kinetic energies.
- Gamma rays are released when an electron makes a transition to a lower energy level in Co-60.
- Gamma rays can be detected using a cloud chamber.
- Alpha particle tracks in a cloud chamber are thicker and longer than those of beta particles.
- In beta minus decay an electron is ejected from the nucleus.
- Half-life is the time for exactly one half of the original number of nuclei to decay.
- Technetium-99m is a radioisotope of half-life 6 h that emits gamma radiation and is used as a tracer in nuclear medicine.
- The line spectrum of hydrogen is evidence for quantised energy levels in the hydrogen atom.
- The longest wavelength in the Balmer series for hydrogen is 656.1 nm.
- The shortest wavelength in the Balmer series for hydrogen is 364.5 nm.
- The wavelengths in the Balmer series become closer together when placed in order from longest to shortest.
- The four longest wavelengths in the Balmer series can be seen by the human eye.
- The energy required to remove an electron from the ground state of the hydrogen atom is 13.6 eV.
- The energy of the photon released when an electron makes a transition from n i =5 to n f =3 is 1.0 eV.
- The shortest wavelength in a certain spectral series for hydrogen is 2.28 μm. The longest wavelength in this series is 7.46 μm.
Modifications of the Bohr Model of the Atom
- The Bohr postulates can be applied to an atom with more than one electron.
- The energy required to remove the electron from the ground state of a helium atom with one electron only is 54.4 eV.
- The difference in intensity of spectral lines is explained using additional quantum numbers to n. This predicts extra states for the electron to exist in. This allowed the development of selection rules and the calculation of transition probabilites.
- The state of the electron in the hydrogen atom is now described by 4 quantum numbers. These are n (1,2,3..), l (0,1,2,..n-1), m (-l, -2,-1,0,1,2,...l) and s (-1/2 or 1/2).