Lesson 3.8.1.1
3.8.1.1 Rutherford scattering Quiz: AQA Physics, Unit 8
20 questions
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Lesson 3.8.1.1, Rutherford scattering: 20 multiple choice questions for the AQA Physics (7408), Unit 8: Nuclear physics (A-level only), written with Revision Ninja.
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The 20 questions
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What did Rutherford's alpha-scattering experiment show about the structure of the atom?
- The nucleus contains only neutrons, which deflect alpha particles on contact
- The atom is a uniform sphere of positive charge with electrons embedded in it
- Electrons orbit at random distances with no fixed structure in the atom
- The atom has a small, dense, positive nucleus that holds most of its mass, with mostly empty space around it
-
Why were a few alpha particles in Rutherford's experiment deflected through large angles?
- They struck heavy electrons, which are more massive than alpha particles
- They approached a small, highly charged nucleus, so the large Coulomb repulsion produced a large deflection
- They were slowed by collisions with neutrons and so reflected backwards
- They passed through dense regions of the electron cloud that deflect them
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What did the plum-pudding model of the atom predict for alpha scattering?
- Alpha particles would be deflected through angles greater than 90 degrees in most cases
- Alpha particles would be absorbed by the atoms and never emerge from the foil
- Alpha particles would be deflected only slightly, since the positive charge was spread thinly over the atom
- Alpha particles would pass through without any interaction with the atoms at all
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Which change would make the closest approach of an alpha particle to a nucleus smaller?
- Reducing the proton number of the target nucleus
- Replacing the target with one that has a larger radius
- Decreasing the alpha particle's initial kinetic energy
- Increasing the alpha particle's initial kinetic energy
-
An alpha particle of kinetic energy 5.0 MeV approaches a gold nucleus (Z = 79) head-on. Estimate its closest approach, using k = 9.0 x 10^9 N m^2 C^-2 and 1 MeV = 1.6 x 10^-13 J.
- 2.3 x 10^-13 m
- 4.6 x 10^-15 m
- 4.6 x 10^-14 m
- 9.1 x 10^-14 m
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Which quantity can be estimated from the closest approach of alpha particles to a nucleus?
- the half-life of the target material
- the radius of the nucleus
- the mass of the electron
- the wavelength of the alpha radiation
-
Why is gold, with Z = 79, a better target than aluminium, with Z = 13, for estimating nuclear size with alpha particles?
- Its larger atomic radius means alpha particles collide with it more often
- Its electrons shield the nucleus, so the alpha particles pass through unchanged
- Its higher nuclear charge gives stronger repulsion, so the alpha particles approach closer before turning back
- Its lower mass means that the alpha particles are deflected more easily
-
An alpha particle has its initial kinetic energy doubled while approaching the same nucleus head-on. How does its closest approach change?
- It is unchanged
- It quadruples
- It doubles
- It halves
-
What is the approximate ratio of the atomic radius to the nuclear radius?
- about 10 times
- about 10^10 times
- about 100 times smaller
- about 10^4 to 10^5
-
A head-on alpha particle has zero speed at its closest approach. What does this show?
- The alpha particle has gained momentum from the nucleus
- The nucleus has absorbed the alpha particle completely
- All its energy has been converted into internal energy of the nucleus
- All its kinetic energy has been converted into electric potential energy of repulsion at that point
-
Which target nucleus gives the greater closest approach for alpha particles of the same energy?
- gold (Z = 79), since closest approach is proportional to nuclear charge
- aluminium (Z = 13), since it is lighter
- both equal, since closest approach depends only on alpha energy
- aluminium, since its electrons repel alpha particles more strongly
-
Which observation in the Geiger-Marsden experiment was most significant in showing that the nucleus is small?
- all alpha particles were deflected by the same small angle
- the foil glowed when struck by alpha particles
- a small number of alpha particles were scattered through large angles, including some close to 180 degrees
- most alpha particles passed straight through the foil with no deflection at all
-
An alpha particle of 5.0 MeV kinetic energy is equal to how many joules? Use 1 MeV = 1.6 x 10^-13 J.
- 8.0 x 10^-6 J
- 1.6 x 10^-19 J
- 3.1 x 10^-13 J
- 8.0 x 10^-13 J
-
A thin gold foil is used in alpha scattering. Why must the foil be thin?
- so that the foil is more likely to absorb every alpha particle
- so that the foil cools the alpha source during the experiment
- so that most alpha particles undergo only a single scattering event, making the results easier to interpret
- so that the foil can be seen clearly through the microscope
-
What order of magnitude is the radius of a gold nucleus?
- about 10^-18 m
- about 10^-6 m
- about 10^-14 m
- about 10^-10 m
-
In a head-on alpha scattering event with an initial kinetic energy of 2.0 MeV on a nucleus of Z = 50, what is the closest approach? Use k = 9.0 x 10^9 N m^2 C^-2.
- 3.6 x 10^-13 m
- 7.2 x 10^-15 m
- 1.8 x 10^-14 m
- 7.2 x 10^-14 m
-
What does the Coulomb equation for closest approach assume?
- that the nucleus mass is the only factor affecting the scattering
- that the alpha particle's momentum is zero at the start because of friction
- that the alpha particle's kinetic energy is entirely converted into electric potential energy at the point of closest approach
- that the alpha particle's kinetic energy is entirely converted into gravitational potential energy
-
A student halves the kinetic energy of an alpha particle approaching a nucleus head-on. By what factor does the closest approach change?
- It halves
- It quadruples
- It doubles
- It is unchanged
-
Electrons diffract from a nucleus, and the intensity pattern against angle gives the nuclear radius. Why is this method useful?
- electrons interact with the nuclear charge through the electromagnetic force, and the pattern minima reveal the size
- electrons are heavier than alpha particles so they reach deeper into the nucleus
- electrons can only reach the outer shell of an atom
- electrons pass through the nucleus and measure its mass directly
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Which is the most reasonable reason why the closest approach estimate gives only an upper limit on the nuclear radius?
- gravitational attraction increases the apparent radius of the nucleus
- the alpha particle is stopped by Coulomb repulsion before it touches the nucleus
- the de Broglie wavelength of the alpha particle makes it appear bigger
- the electrons add to the apparent radius of the nucleus
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