1. What differs between isotopes of the same element?
- Number of protons
- Sign of the electron charge
- Number of neutrons
Check the answer and reasoning
Number of neutrons
The proton number identifies the element.
Physics / IGCSE
Separate atomic structure from random radioactive change.
An atom has a small nucleus containing protons and neutrons, with electrons outside it. Isotopes have the same proton number but different neutron numbers, so they are forms of the same element.
Radioactive decay is random for an individual nucleus. A large sample has a predictable statistical pattern: activity halves in each half-life. Radiation can ionise matter, so exposure requires controlled professional procedures.
An atom contains a small positively charged nucleus and surrounding electrons. Proton number identifies the element; nucleon number counts protons plus neutrons. Isotopes share proton number but differ in neutrons. A neutral atom has equal proton and electron numbers; removing an electron makes an ion, not a new isotope. Alpha-particle scattering supports a small concentrated nucleus rather than a uniform distribution of positive charge.
Alpha radiation consists of helium nuclei, beta-minus radiation of electrons from nuclear change, and gamma radiation of high-energy photons. Alpha emission reduces nucleon number by four and proton number by two; beta-minus leaves nucleon number unchanged and raises proton number by one. Gamma emission changes nuclear energy without changing these counts. Penetration and ionising ability differ, so shielding and exposure considerations depend on radiation type.
A detector records some radiation interactions, not necessarily every decay in a source. Background comes from environmental and cosmic sources and varies statistically. Measure it for a suitable interval and subtract its count rate from the total to obtain a corrected count rate. A total of 150 counts/min with background 30 counts/min gives 120 counts/min corrected. Converting that result to activity requires information about detection efficiency and geometry.
One nucleus has an unpredictable decay time, but many similar nuclei show a regular statistical trend. After each half-life, the expected number undecayed and the activity each halve. Corrected count rate can track that trend when detection conditions stay unchanged. Three half-lives leave one eighth, not one third. Small samples and short count intervals show fluctuations, so a single reading rarely gives an exact half-life.
Fission splits a heavy nucleus and can produce neutrons capable of triggering further fissions. Fusion joins light nuclei under suitable conditions. Energy release corresponds to a reduction in total rest mass; it does not mean all matter disappears. Exposure should be minimised through suitable time, distance, shielding and controlled procedures. Contamination means radioactive material has spread; irradiation means radiation reaches something and does not necessarily make it radioactive. Never handle sources independently.
Yes. Different radiation types, shielding, distances and detector efficiencies can produce different recorded rates even if the sources undergo the same number of decays per second.
n is the number of elapsed half-lives.
A source has measured count rate 800 counts/min. With negligible background and unchanged detection conditions, what is expected after two half-lives?
800 → 400 → 200 counts/min.
Model random decay by repeatedly removing coins that land heads; graph the remaining number. Use no radioactive materials.
Compare atomic identity with nuclear change, then view statistical decay. Simulations are educational representations, not instructions for sourcing, shielding or handling radioactive materials.
Number of neutrons
The proton number identifies the element.
200 counts/min
800 → 400 → 200 counts/min.
Subtract background to find the corrected source count rate.
A detector records both source and background; corrected count rate is not necessarily the full activity because detection efficiency matters.