DP Physics Questionbank
Option D: Astrophysics (Additional higher level option topics)
Description
Overview of the essential ideas for this option
D.4: The laws of nuclear physics applied to nuclear fusion processes inside stars determine the production of all elements up to iron.
D.5: The modern field of cosmology uses advanced experimental and observational techniques to collect data with an unprecedented degree of precision and as a result very surprising and detailed conclusions about the structure of the universe have been reached.
Directly related questions
- 16N.3.HL.TZ0.24a: Describe how some white dwarf stars become type Ia supernovae.
- 16N.3.HL.TZ0.24b: Hence, explain why a type Ia supernova is used as a standard candle.
-
16N.3.HL.TZ0.25a:
Calculate the rotation velocity of stars 4.0 kpc from the centre of the galaxy. The average density of the galaxy is 5.0 × 10–21 kg m–3.
- 16N.3.HL.TZ0.25b: Explain why the rotation curves are evidence for the existence of dark matter.
- 16N.3.HL.TZ0.24c: Explain how the observation of type Ia supernovae led to the hypothesis that dark energy exists.
-
17M.3.HL.TZ1.17a:
The graph shows the variation with time t of the cosmic scale factor R in the flat model of the universe in which dark energy is ignored.
On the axes above draw a graph to show the variation of R with time, when dark energy is present.
-
17M.3.HL.TZ1.17b.ii:
The density of dark energy is ρΛc2 where ρΛ = ρc – ρm. Calculate the amount of dark energy in 1 m3 of space.
-
17M.3.HL.TZ2.20a:
Describe what is meant by dark matter.
-
17M.3.HL.TZ1.16a:
Outline, with reference to star formation, what is meant by the Jeans criterion.
-
17M.3.HL.TZ1.16b:
In the proton–proton cycle, four hydrogen nuclei fuse to produce one nucleus of helium releasing a total of 4.3 × 10–12 J of energy. The Sun will spend 1010 years on the main sequence. It may be assumed that during this time the Sun maintains a constant luminosity of 3.8 × 1026 W.
Show that the total mass of hydrogen that is converted into helium while the Sun is on the main sequence is 2 × 1029 kg. -
17M.3.HL.TZ1.16c:
Massive stars that have left the main sequence have a layered structure with different chemical elements in different layers. Discuss this structure by reference to the nuclear reactions taking place in such stars.
-
17M.3.HL.TZ2.19a.ii:
The present temperature of the CMB is 2.8 K. This radiation was emitted when the universe was smaller by a factor of 1100. Estimate the temperature of the CMB at the time of its emission.
-
17M.3.HL.TZ2.19b:
State how the anisotropies in the CMB distribution are interpreted.
-
17M.3.HL.TZ2.20c:
Curve A shows the actual rotation curve of a nearby galaxy. Curve B shows the predicted rotation curve based on the visible stars in the galaxy.
Explain how curve A provides evidence for dark matter.
-
17M.3.HL.TZ1.17b.i:
The density of the observable matter in the universe is only 0.05 ρc. Suggest how the remaining 0.27 ρc is accounted for.
-
17M.3.HL.TZ2.19a.i:
Derive, using the concept of the cosmological origin of redshift, the relation
T
between the temperature T of the cosmic microwave background (CMB) radiation and the cosmic scale factor R.
-
17M.3.HL.TZ2.20b:
The distribution of mass in a spherical system is such that the density ρ varies with distance r from the centre as
ρ =
where k is a constant.
Show that the rotation curve of this system is described by
v = constant.
- 20N.3.HL.TZ0.22e: Eta Aquilae A was on the main sequence before it became a variable star. Compare, without...
-
20N.3.HL.TZ0.24b:
Identify two possible causes of the anisotropies in (a).
- 20N.3.HL.TZ0.23: In 2017, two neutron stars were observed to merge, forming a black hole. The material released...
- 20N.3.HL.TZ0.21c: Hubble originally linked galactic redshift to a Doppler effect arising from galactic recession....
- 20N.3.HL.TZ0.24a: State the nature of the anisotropies observed in the CMB radiation.
-
17N.3.HL.TZ0.20a:
The Sun is a second generation star. Outline, with reference to the Jeans criterion (MJ), how the Sun is likely to have been formed.
-
17N.3.HL.TZ0.20c:
Show that the critical density of the universe is
where H is the Hubble parameter and G is the gravitational constant.
-
17N.3.HL.TZ0.20b:
Suggest how fluctuations in the cosmic microwave background (CMB) radiation are linked to the observation that galaxies collide.
-
18M.3.HL.TZ1.19a:
The mass of visible matter in the galaxy is M.
Show that for stars where r > R0 the velocity of orbit is v = .
-
18M.3.HL.TZ1.18a:
Describe the formation of a type Ia supernova.
-
18M.3.HL.TZ1.19c:
Explain, using the equation in (a) and the graphs, why the presence of visible matter alone cannot account for the velocity of stars when r > R0.
-
18M.3.HL.TZ1.18b.i:
Show that the distance to the supernova is approximately 3.1 × 1018 m.
-
18M.3.HL.TZ1.19b:
Draw on the axes the observed variation with r of the orbital speed v of stars in a galaxy.
-
18M.3.HL.TZ1.18b.ii:
State one assumption made in your calculation.
-
18M.3.HL.TZ2.18a:
Outline, with reference to the Jeans criterion, why a cold dense gas cloud is more likely to form new stars than a hot diffuse gas cloud.
-
18M.3.HL.TZ2.18b:
Explain how neutron capture can produce elements with an atomic number greater than iron.
-
18M.3.HL.TZ2.19a:
Explain the evidence that indicates the location of dark matter in galaxies.
-
18M.3.HL.TZ2.19b:
Outline why a hypothesis of dark energy has been developed.
- 21N.1.SL.TZ0.30: Which is correct for a black-body radiator? A. The power it emits from a unit surface area...
-
18N.3.HL.TZ0.21b:
The present temperature of the cosmic microwave background (CMB) radiation is 3 K. Estimate the size of the universe relative to the present size of the universe when the temperature of the CMB was 300 K.
- 18N.3.HL.TZ0.17c: The Great Nebula is located in Orion. Describe, using the Jeans criterion, the...
- 18N.3.HL.TZ0.20a: Outline what is meant by dark energy.
- 18N.3.HL.TZ0.20b: State two candidates for dark matter.
-
18N.3.HL.TZ0.21a:
Show that the temperature of the universe is inversely proportional to the cosmic scale factor.
- 19M.3.HL.TZ2.21b: Describe the r process which occurs during type II supernovae nucleosynthesis.
- 19M.3.HL.TZ1.19a.i: Describe the mechanism of formation of type I a supernovae.
- 19M.3.HL.TZ1.20a: Light from distant galaxies is redshifted. Explain the cosmological origin of this redshift.
-
19M.3.HL.TZ1.20b.ii:
Compare and contrast, the variation with time of the temperature of the cosmic background (CMB) radiation, for the two models from the present time onward.
- 19M.3.HL.TZ1.20b.i: Draw, on the axes, a graph to show the variation with time of the cosmic scale factor R for the...
-
19M.3.HL.TZ1.19a.ii:
Describe the mechanism of formation of type II supernovae.
- 19M.3.HL.TZ2.21a: Explain the formation of a type I a supernova which enables the star to be used as a standard...
-
19M.3.HL.TZ2.22b:
At critical density there is zero total energy. Show that the critical density of the universe is: .
-
19M.3.HL.TZ2.22a:
Justify that the total energy of this particle is .
- 19M.3.HL.TZ2.22c: The accepted value for the Hubble constant is 2.3 × 10−18 s−1. Estimate the critical density of...
-
19N.3.HL.TZ0.17a:
Proxima Centauri is a main sequence star with a mass of 0.12 solar masses.
Estimate .
- 19N.3.HL.TZ0.17b: Describe why iron is the heaviest element that can be produced by nuclear fusion processes inside...
- 19N.3.HL.TZ0.16b(iii): It is estimated that less than 20 % of the matter in the universe is observable. Discuss how...
- 19N.3.HL.TZ0.16b(i): State what is meant by the critical density.
-
19N.3.HL.TZ0.16b(ii):
Calculate the density of matter in the universe, using the Hubble constant 70 km s–1 Mpc–1.
-
19N.3.HL.TZ0.17c:
Discuss one process by which elements heavier than iron are formed in stars.
Sub sections and their related questions
D.4 – Stellar processes (HL only)
- 16N.3.HL.TZ0.24a: Describe how some white dwarf stars become type Ia supernovae.
- 16N.3.HL.TZ0.24b: Hence, explain why a type Ia supernova is used as a standard candle.
- 16N.3.HL.TZ0.24c: Explain how the observation of type Ia supernovae led to the hypothesis that dark energy exists.
-
17M.3.HL.TZ1.16a:
Outline, with reference to star formation, what is meant by the Jeans criterion.
-
17M.3.HL.TZ1.16b:
In the proton–proton cycle, four hydrogen nuclei fuse to produce one nucleus of helium releasing a total of 4.3 × 10–12 J of energy. The Sun will spend 1010 years on the main sequence. It may be assumed that during this time the Sun maintains a constant luminosity of 3.8 × 1026 W.
Show that the total mass of hydrogen that is converted into helium while the Sun is on the main sequence is 2 × 1029 kg. -
17M.3.HL.TZ1.16c:
Massive stars that have left the main sequence have a layered structure with different chemical elements in different layers. Discuss this structure by reference to the nuclear reactions taking place in such stars.
-
17N.3.HL.TZ0.20a:
The Sun is a second generation star. Outline, with reference to the Jeans criterion (MJ), how the Sun is likely to have been formed.
-
18M.3.HL.TZ1.18a:
Describe the formation of a type Ia supernova.
-
18M.3.HL.TZ1.18b.i:
Show that the distance to the supernova is approximately 3.1 × 1018 m.
-
18M.3.HL.TZ1.18b.ii:
State one assumption made in your calculation.
-
18M.3.HL.TZ2.18a:
Outline, with reference to the Jeans criterion, why a cold dense gas cloud is more likely to form new stars than a hot diffuse gas cloud.
-
18M.3.HL.TZ2.18b:
Explain how neutron capture can produce elements with an atomic number greater than iron.
- 18N.3.HL.TZ0.17c: The Great Nebula is located in Orion. Describe, using the Jeans criterion, the...
- 19M.3.HL.TZ2.21b: Describe the r process which occurs during type II supernovae nucleosynthesis.
- 19M.3.HL.TZ1.19a.i: Describe the mechanism of formation of type I a supernovae.
-
19M.3.HL.TZ1.19a.ii:
Describe the mechanism of formation of type II supernovae.
- 19M.3.HL.TZ2.21a: Explain the formation of a type I a supernova which enables the star to be used as a standard...
-
19N.3.HL.TZ0.17a:
Proxima Centauri is a main sequence star with a mass of 0.12 solar masses.
Estimate .
- 19N.3.HL.TZ0.17b: Describe why iron is the heaviest element that can be produced by nuclear fusion processes inside...
-
19N.3.HL.TZ0.17c:
Discuss one process by which elements heavier than iron are formed in stars.
- 20N.3.HL.TZ0.22e: Eta Aquilae A was on the main sequence before it became a variable star. Compare, without...
- 20N.3.HL.TZ0.23: In 2017, two neutron stars were observed to merge, forming a black hole. The material released...
- 21N.1.SL.TZ0.30: Which is correct for a black-body radiator? A. The power it emits from a unit surface area...
D.5 – Further cosmology (HL only)
-
16N.3.HL.TZ0.25a:
Calculate the rotation velocity of stars 4.0 kpc from the centre of the galaxy. The average density of the galaxy is 5.0 × 10–21 kg m–3.
- 16N.3.HL.TZ0.25b: Explain why the rotation curves are evidence for the existence of dark matter.
-
17M.3.HL.TZ1.17a:
The graph shows the variation with time t of the cosmic scale factor R in the flat model of the universe in which dark energy is ignored.
On the axes above draw a graph to show the variation of R with time, when dark energy is present.
-
17M.3.HL.TZ1.17b.i:
The density of the observable matter in the universe is only 0.05 ρc. Suggest how the remaining 0.27 ρc is accounted for.
-
17M.3.HL.TZ1.17b.ii:
The density of dark energy is ρΛc2 where ρΛ = ρc – ρm. Calculate the amount of dark energy in 1 m3 of space.
-
17M.3.HL.TZ2.19a.i:
Derive, using the concept of the cosmological origin of redshift, the relation
T
between the temperature T of the cosmic microwave background (CMB) radiation and the cosmic scale factor R.
-
17M.3.HL.TZ2.19a.ii:
The present temperature of the CMB is 2.8 K. This radiation was emitted when the universe was smaller by a factor of 1100. Estimate the temperature of the CMB at the time of its emission.
-
17M.3.HL.TZ2.19b:
State how the anisotropies in the CMB distribution are interpreted.
-
17M.3.HL.TZ2.20a:
Describe what is meant by dark matter.
-
17M.3.HL.TZ2.20b:
The distribution of mass in a spherical system is such that the density ρ varies with distance r from the centre as
ρ =
where k is a constant.
Show that the rotation curve of this system is described by
v = constant.
-
17M.3.HL.TZ2.20c:
Curve A shows the actual rotation curve of a nearby galaxy. Curve B shows the predicted rotation curve based on the visible stars in the galaxy.
Explain how curve A provides evidence for dark matter.
-
17N.3.HL.TZ0.20b:
Suggest how fluctuations in the cosmic microwave background (CMB) radiation are linked to the observation that galaxies collide.
-
17N.3.HL.TZ0.20c:
Show that the critical density of the universe is
where H is the Hubble parameter and G is the gravitational constant.
-
18M.3.HL.TZ1.19a:
The mass of visible matter in the galaxy is M.
Show that for stars where r > R0 the velocity of orbit is v = .
-
18M.3.HL.TZ1.19b:
Draw on the axes the observed variation with r of the orbital speed v of stars in a galaxy.
-
18M.3.HL.TZ1.19c:
Explain, using the equation in (a) and the graphs, why the presence of visible matter alone cannot account for the velocity of stars when r > R0.
-
18M.3.HL.TZ2.19a:
Explain the evidence that indicates the location of dark matter in galaxies.
-
18M.3.HL.TZ2.19b:
Outline why a hypothesis of dark energy has been developed.
- 18N.3.HL.TZ0.20a: Outline what is meant by dark energy.
- 18N.3.HL.TZ0.20b: State two candidates for dark matter.
-
18N.3.HL.TZ0.21a:
Show that the temperature of the universe is inversely proportional to the cosmic scale factor.
-
18N.3.HL.TZ0.21b:
The present temperature of the cosmic microwave background (CMB) radiation is 3 K. Estimate the size of the universe relative to the present size of the universe when the temperature of the CMB was 300 K.
- 19M.3.HL.TZ1.20a: Light from distant galaxies is redshifted. Explain the cosmological origin of this redshift.
- 19M.3.HL.TZ1.20b.i: Draw, on the axes, a graph to show the variation with time of the cosmic scale factor R for the...
-
19M.3.HL.TZ1.20b.ii:
Compare and contrast, the variation with time of the temperature of the cosmic background (CMB) radiation, for the two models from the present time onward.
-
19M.3.HL.TZ2.22a:
Justify that the total energy of this particle is .
-
19M.3.HL.TZ2.22b:
At critical density there is zero total energy. Show that the critical density of the universe is: .
- 19M.3.HL.TZ2.22c: The accepted value for the Hubble constant is 2.3 × 10−18 s−1. Estimate the critical density of...
- 19N.3.HL.TZ0.16b(i): State what is meant by the critical density.
-
19N.3.HL.TZ0.16b(ii):
Calculate the density of matter in the universe, using the Hubble constant 70 km s–1 Mpc–1.
- 19N.3.HL.TZ0.16b(iii): It is estimated that less than 20 % of the matter in the universe is observable. Discuss how...
- 20N.3.HL.TZ0.21c: Hubble originally linked galactic redshift to a Doppler effect arising from galactic recession....
- 20N.3.HL.TZ0.24a: State the nature of the anisotropies observed in the CMB radiation.
-
20N.3.HL.TZ0.24b:
Identify two possible causes of the anisotropies in (a).
- 21N.1.SL.TZ0.30: Which is correct for a black-body radiator? A. The power it emits from a unit surface area...