The Atomic NucleusThe nucleus of an atom contains nucleons: protons and neutrons. Protons repel each other via the Coulomb force but over a very short range (femtometres) there exists a very strong force called the strong nuclear force. This binds the nucleons together into a nucleus. Nuclei are typically femtometres in diameter  (a femtometre (fm) is 10^{15}m). To view a scaled diagram of an atom on your computer screen with a nucleus of 1 cm diameter in the centre you would need a screen of 1km diameter to show the full graphic! The nucleus is tiny compared to a whole atom. It occupies one part in 100,000,000,000,000 of the atomic volume The number of protons (Z) determines the chemical properties of the atom  which element it belongs to  it is called the proton number or atomic number. The number of neutrons (N) affects its physical properties  which isotope of the element it belongs to. The mass number (A) or nucleon number is the number of protons plus the number of neutrons The specific charge of a nucleus is the total charge of the nucleons (in coulombs) divided by the total mass of the nucleons (in kilograms). Specific charge is measured in C^{1}kg Various types of scattering experiments suggest that nuclei are roughly spherical and appear to have essentially the same average density. This is studied at A level and is deduced from the following equation  where r is the radius of the nucleus of mass number A.: This equation can be deduced from the following reasoning: The mass of the nucleus will depend on A  the number of nucleons in the nucleus  as they have virtually the same mass : Nuclear mass = Am where
Assuming the nucleus is spherical we have a volume: V = ^{4}/_{3}πr^{3} Density = mass / volume So, ρ = Am/(^{4}/_{3}πr^{3}) ρ = 3Am/(4πr^{3}) m and are constant  there is therefore a constant value of 3m/(4π) and we can say that: Density is proprtional to A/r^{3} Rearranging this we get that r is proportional to the density divided by the cube root of A If we call the constant of proportionality r_{o} we get the above equation. If r is plotted against A^{1/3} a straight line is obtained  the gradient of it is the constant r_{o}  but the relationship is best for large values of A so if you use small values this does not work too well!
To show that nuclear density is independent of A in other words that all nuclei have the same density  or uniform densityLet the volume of a nucleus be V the mass of the nucleus be M and the mass of a nucleon be m V = ^{4}/_{3}r^{3} ρ = M/V So, M = ^{4}/_{3}r^{3}ρ Let's replace the r^{3} in this expression by using the equation above for r so, r^{3} = r_{o}^{3}A M = ^{4}/_{3} r_{o}^{3}A ρ but M = Am So, Am = ^{4}/_{3}r_{o}^{3}A Therefore, Rearranging we get, ρ = 3m/(4r_{o}^{3} ) This means that the density does not depend on A or on r  it is related to constant values  it is therefore a constant value and uniform. Data relating to nuclear sizeThe most definitive information about nuclear sizes comes from electron scattering experiments. If we compare calculated and experimental radii for nuclei we find that that there is an area around the edge of the nucleus where the density of nuclear matter decreases toward zero  but that the central part is roughly of constant density. So the nucleus cannot be thought of as just a hard sphere. The fact that the nuclear density is independent of the details of neutron number or proton number suggests that the force between the particles is essentially the same whether they are protons or neutrons. This agrees with other evidence that the strong force is the same between any pair of nucleons.
Techniques employed to study the nucleus

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