AQA · A-Level · Physics

    Course version: 7408 · Version from Sept 2016

    Conservation of strangeness in strong interactions.

    Full specification wording

    Classification of particles: Conservation of strangeness in strong interactions.

    In a strong interaction the total strangeness of the reacting particles equals the total strangeness of the products.

    Checked against the AQA 7408 specification (opens in a new tab) on .

    • Point 13 of 15
    • 4 key terms

    Study notes

    From the checked teaching notes for this specification point.

    The idea

    In a strong interaction the total strangeness of the reacting particles equals the total strangeness of the products. This rule follows from the fact that the strong force acts on quarks and cannot change a strange quark into a non-strange quark or create a strange quark without its antiquark. For example, in π⁻ + p → K⁰ + Λ⁰ the initial strangeness is 0 + 0 = 0, while the products give +1 + (−1) = 0, so the reaction is allowed. In contrast, a reaction such as p + p → p + Σ⁺ would have initial strangeness 0 and final strangeness −1, so it cannot proceed by the strong interaction. Strangeness is not conserved in weak interactions, which is why strange particles can decay singly, for example Λ⁰ → p + π⁻.

    What earns the marks

    • Total strangeness is conserved in strong interactions, so the sum of s values before equals the sum after.
    • Strong interactions cannot alter quark flavour, so a strange quark remains a strange quark and a strange antiquark remains a strange antiquark.
    • A reaction with unequal total strangeness on the two sides is forbidden as a strong interaction.
    • Weak interactions do not conserve strangeness, so they provide the route by which strange particles decay.
    • Checking strangeness conservation is a standard test for whether a proposed reaction can occur via the strong force.
    • The rule applies to all strongly interacting particles in the reaction, including mesons and baryons.

    Common mistakes and how to put them right

    • Applying strangeness conservation to every interaction, including weak decays.

      Put it right by identifying the interaction type first and only requiring conservation for strong and electromagnetic processes.

    • Adding strangeness values without regard to the sign carried by antiparticles.

      Put it right by assigning s = +1 to a strange antiquark and s = −1 to a strange quark.

    • Assuming that a reaction is allowed simply because charge and baryon number balance.

      Put it right: Also checking strangeness when strange particles are present.

    Exam tips

    • Label each particle with its strangeness value before and after the arrow, then compare the two totals in one line.
    • If a proposed reaction fails strangeness conservation, state that it cannot occur by the strong interaction rather than saying it is impossible in all circumstances.
    • Link the conservation check to the interaction type named in the question, since weak processes are treated differently.

    Try the lesson

    The start of the Classification of particles: Conservation of strangeness in strong interactions. lesson, made from checked teaching notes for this specification point.

    Have a go first

    Which of the following quantities is always conserved in strong interactions but can change in weak interactions?

    Listen

    In a strong interaction the total strangeness of the reacting particles equals the total strangeness of the products. This rule follows from the fact that the strong force acts on quarks and cannot change a strange quark into a non-strange quark or create a strange quark without its antiquark. For example, in π⁻ + p → K⁰ + Λ⁰ the initial strangeness is 0 + 0 = 0, while the products give +1 + (−1) = 0, so the reaction is allowed. In contrast, a reaction such as p + p → p + Σ⁺ would have initial strangeness 0 and final strangeness −1, so it cannot proceed by the strong interaction. Strangeness is not conserved in weak interactions, which is why strange particles can decay singly, for example Λ⁰ → p + π⁻. A strong answer earns marks for these points. Total strangeness is conserved in strong interactions, so the sum of s values before equals the sum after. Strong interactions cannot alter quark flavour, so a strange quark remains a strange quark and a strange antiquark remains a strange antiquark. A reaction with unequal total strangeness on the two sides is forbidden as a strong interaction. Weak interactions do not conserve strangeness, so they provide the route by which strange particles decay. A common slip: Applying strangeness conservation to every interaction, including weak decays. Instead, identifying the interaction type first and only requiring conservation for strong and electromagnetic processes. Exam tip: Label each particle with its strangeness value before and after the arrow, then compare the two totals in one line.

    Key words

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    Conservation of strangeness

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    Strong interactions

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    Weak interactions

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    Particle reaction feasibility

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    See every definition
    Conservation of strangeness
    In a strong interaction the total strangeness of the reacting particles equals the total strangeness of the products.
    Strong interactions
    These act on quarks and cannot change a strange quark into a non-strange quark or create a strange quark without its antiquark.
    Weak interactions
    These do not conserve strangeness, which is why strange particles can decay singly.
    Particle reaction feasibility
    A reaction with unequal total strangeness on the two sides is forbidden as a strong interaction.

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