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A.8 Superconducting metals and X-ray crystallography (HL only)
Description
[N/A]Directly related questions
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17N.3.hl.TZ0.8a:
Calculate the total number of cobalt atoms within its unit cell.
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17N.3.hl.TZ0.8a:
Calculate the total number of cobalt atoms within its unit cell.
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17N.3.hl.TZ0.a:
Calculate the total number of cobalt atoms within its unit cell.
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17N.3.hl.TZ0.6b:
Explain why Type 2 superconductors are generally more useful than Type 1.
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17N.3.hl.TZ0.6b:
Explain why Type 2 superconductors are generally more useful than Type 1.
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17N.3.hl.TZ0.b:
Explain why Type 2 superconductors are generally more useful than Type 1.
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17N.3.hl.TZ0.8b.i:
The atomic radius, r, of cobalt is 1.18 × 10–8 cm. Determine the edge length, in cm, of the unit cell, a, using the second diagram.
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17N.3.hl.TZ0.8b.i:
The atomic radius, r, of cobalt is 1.18 × 10–8 cm. Determine the edge length, in cm, of the unit cell, a, using the second diagram.
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17N.3.hl.TZ0.b.i:
The atomic radius, r, of cobalt is 1.18 × 10–8 cm. Determine the edge length, in cm, of the unit cell, a, using the second diagram.
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17N.3.hl.TZ0.8b.ii:
Determine a value for the density of cobalt, in g cm–3, using data from sections 2 and 6 of the data booklet and your answers from (a) and (b) (i).
If you did not obtain an answer to (b) (i), use 3.00 × 10–8 cm but this is not the correct answer.
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17N.3.hl.TZ0.8b.ii:
Determine a value for the density of cobalt, in g cm–3, using data from sections 2 and 6 of the data booklet and your answers from (a) and (b) (i).
If you did not obtain an answer to (b) (i), use 3.00 × 10–8 cm but this is not the correct answer.
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17N.3.hl.TZ0.b.ii:
Determine a value for the density of cobalt, in g cm–3, using data from sections 2 and 6 of the data booklet and your answers from (a) and (b) (i).
If you did not obtain an answer to (b) (i), use 3.00 × 10–8 cm but this is not the correct answer.
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18M.3.hl.TZ2.4a.i:
Deduce the number of atoms per unit cell in vanadium.
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18M.3.hl.TZ2.4a.i:
Deduce the number of atoms per unit cell in vanadium.
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18M.3.hl.TZ2.a.i:
Deduce the number of atoms per unit cell in vanadium.
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18M.3.hl.TZ1.5c:
When X-rays of wavelength 0.154 nm are directed at a crystal of aluminium, the first order diffraction pattern is observed at 18°. Determine the separation of layers of aluminium atoms in the crystal, in m, using section 1 of the data booklet.
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18M.3.hl.TZ1.5c:
When X-rays of wavelength 0.154 nm are directed at a crystal of aluminium, the first order diffraction pattern is observed at 18°. Determine the separation of layers of aluminium atoms in the crystal, in m, using section 1 of the data booklet.
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18M.3.hl.TZ1.c:
When X-rays of wavelength 0.154 nm are directed at a crystal of aluminium, the first order diffraction pattern is observed at 18°. Determine the separation of layers of aluminium atoms in the crystal, in m, using section 1 of the data booklet.
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18M.3.hl.TZ1.5d.i:
Deduce what the shape of the graph indicates about aluminium.
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18M.3.hl.TZ1.5d.i:
Deduce what the shape of the graph indicates about aluminium.
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18M.3.hl.TZ1.d.i:
Deduce what the shape of the graph indicates about aluminium.
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18M.3.hl.TZ2.4a.ii:
Calculate the expected first order diffraction pattern angle, in degrees, if x-rays of wavelength 150 pm are directed at a crystal of vanadium. Assume the edge length of the crystal to be the same as separation of layers of vanadium atoms found by x-ray diffraction. Use section 1 of the data booklet.
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18M.3.hl.TZ2.4a.ii:
Calculate the expected first order diffraction pattern angle, in degrees, if x-rays of wavelength 150 pm are directed at a crystal of vanadium. Assume the edge length of the crystal to be the same as separation of layers of vanadium atoms found by x-ray diffraction. Use section 1 of the data booklet.
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18M.3.hl.TZ2.a.ii:
Calculate the expected first order diffraction pattern angle, in degrees, if x-rays of wavelength 150 pm are directed at a crystal of vanadium. Assume the edge length of the crystal to be the same as separation of layers of vanadium atoms found by x-ray diffraction. Use section 1 of the data booklet.
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18M.3.hl.TZ2.4a.iv:
Determine the volume, in cm3, of a vanadium unit cell.
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18M.3.hl.TZ2.4a.iv:
Determine the volume, in cm3, of a vanadium unit cell.
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18M.3.hl.TZ2.a.iv:
Determine the volume, in cm3, of a vanadium unit cell.
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18M.3.hl.TZ1.5d.ii:
Outline why the resistance of aluminium increases above 1.2 K.
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18M.3.hl.TZ1.5d.ii:
Outline why the resistance of aluminium increases above 1.2 K.
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18M.3.hl.TZ1.d.ii:
Outline why the resistance of aluminium increases above 1.2 K.
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18M.3.hl.TZ2.4a.v:
Determine the density, in g cm−3, of vanadium by using your answers to (a)(i), (a)(iii) and (a)(iv).
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18M.3.hl.TZ2.4a.v:
Determine the density, in g cm−3, of vanadium by using your answers to (a)(i), (a)(iii) and (a)(iv).
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18M.3.hl.TZ2.a.v:
Determine the density, in g cm−3, of vanadium by using your answers to (a)(i), (a)(iii) and (a)(iv).
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18N.3.hl.TZ0.5a.ii:
Calculate the number of atoms per unit cell of gold, showing your working.
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18N.3.hl.TZ0.5a.ii:
Calculate the number of atoms per unit cell of gold, showing your working.
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18N.3.hl.TZ0.a.ii:
Calculate the number of atoms per unit cell of gold, showing your working.
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18N.3.hl.TZ0.5b:
The edge length of the gold unit cell is 4.08 × 10‒8 cm.
Determine the density of gold in g cm‒3, using sections 2 and 6 of the data booklet.
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18N.3.hl.TZ0.5b:
The edge length of the gold unit cell is 4.08 × 10‒8 cm.
Determine the density of gold in g cm‒3, using sections 2 and 6 of the data booklet.
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18N.3.hl.TZ0.b:
The edge length of the gold unit cell is 4.08 × 10‒8 cm.
Determine the density of gold in g cm‒3, using sections 2 and 6 of the data booklet.
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19M.3.hl.TZ1.3e:
Lithium forms a crystalline lattice with the unit cell structure shown below.
X-ray diffraction shows that the length of the edge of the unit cell is 3.51 × 10−8 cm.
Determine the density of lithium, in g cm−3, using sections 2 and 6 of the data booklet.
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19M.3.hl.TZ1.3e:
Lithium forms a crystalline lattice with the unit cell structure shown below.
X-ray diffraction shows that the length of the edge of the unit cell is 3.51 × 10−8 cm.
Determine the density of lithium, in g cm−3, using sections 2 and 6 of the data booklet.
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19M.3.hl.TZ1.e:
Lithium forms a crystalline lattice with the unit cell structure shown below.
X-ray diffraction shows that the length of the edge of the unit cell is 3.51 × 10−8 cm.
Determine the density of lithium, in g cm−3, using sections 2 and 6 of the data booklet.
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19M.3.hl.TZ1.3d(ii):
At very low temperatures, lithium atoms enhance the phonon binding of electrons in graphene suggesting the formation of Cooper pairs.
Explain how Cooper pairs are formed.
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19M.3.hl.TZ1.3d(ii):
At very low temperatures, lithium atoms enhance the phonon binding of electrons in graphene suggesting the formation of Cooper pairs.
Explain how Cooper pairs are formed.
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19M.3.hl.TZ1.d(ii):
At very low temperatures, lithium atoms enhance the phonon binding of electrons in graphene suggesting the formation of Cooper pairs.
Explain how Cooper pairs are formed.
- 19N.3.hl.TZ0.4a(i): Outline how resistance to electric currents occurs in metals.
- 19N.3.hl.TZ0.4a(i): Outline how resistance to electric currents occurs in metals.
- 19N.3.hl.TZ0.a(i): Outline how resistance to electric currents occurs in metals.
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18M.3.hl.TZ1.5b:
The diagram illustrates the crystal structure of aluminium metal with the unit cell indicated. Outline the significance of the unit cell.
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18M.3.hl.TZ1.5b:
The diagram illustrates the crystal structure of aluminium metal with the unit cell indicated. Outline the significance of the unit cell.
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18M.3.hl.TZ1.b:
The diagram illustrates the crystal structure of aluminium metal with the unit cell indicated. Outline the significance of the unit cell.
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18M.3.hl.TZ2.4a.iii:
Calculate the average mass, in g, of a vanadium atom by using sections 2 and 6 of the data booklet.
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18M.3.hl.TZ2.4a.iii:
Calculate the average mass, in g, of a vanadium atom by using sections 2 and 6 of the data booklet.
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18M.3.hl.TZ2.a.iii:
Calculate the average mass, in g, of a vanadium atom by using sections 2 and 6 of the data booklet.
- 18N.3.hl.TZ0.5a.i: State the name of the crystal structure of gold.
- 18N.3.hl.TZ0.5a.i: State the name of the crystal structure of gold.
- 18N.3.hl.TZ0.a.i: State the name of the crystal structure of gold.
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19M.3.hl.TZ1.3d(i):
Lithium has shown some superconductive properties when doped into graphene or when under high pressure. Under high pressure, however, the Meissner effect is absent.
Describe the Meissner effect.
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19M.3.hl.TZ1.3d(i):
Lithium has shown some superconductive properties when doped into graphene or when under high pressure. Under high pressure, however, the Meissner effect is absent.
Describe the Meissner effect.
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19M.3.hl.TZ1.d(i):
Lithium has shown some superconductive properties when doped into graphene or when under high pressure. Under high pressure, however, the Meissner effect is absent.
Describe the Meissner effect.
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19M.3.hl.TZ2.6a:
State the number of atoms in the unit cell.
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19M.3.hl.TZ2.6a:
State the number of atoms in the unit cell.
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19M.3.hl.TZ2.a:
State the number of atoms in the unit cell.
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19M.3.hl.TZ2.6b:
Determine the density of calcium, in g cm−3, using section 2 of the data booklet.
Ar = 40.08; metallic radius (r) = 1.97 × 10−10 m
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19M.3.hl.TZ2.6b:
Determine the density of calcium, in g cm−3, using section 2 of the data booklet.
Ar = 40.08; metallic radius (r) = 1.97 × 10−10 m
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19M.3.hl.TZ2.b:
Determine the density of calcium, in g cm−3, using section 2 of the data booklet.
Ar = 40.08; metallic radius (r) = 1.97 × 10−10 m
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19M.3.hl.TZ2.7a:
State what is meant by a superconductor.
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19M.3.hl.TZ2.7a:
State what is meant by a superconductor.
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19M.3.hl.TZ2.a:
State what is meant by a superconductor.
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19M.3.hl.TZ2.18b:
Outline one approach to controlling industrial emissions of carbon dioxide.
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19M.3.hl.TZ2.18b:
Outline one approach to controlling industrial emissions of carbon dioxide.
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19M.3.hl.TZ2.b:
Outline one approach to controlling industrial emissions of carbon dioxide.
- 19N.3.hl.TZ0.4a(ii): Suggest why the resistance of metals increases with temperature.
- 19N.3.hl.TZ0.4a(ii): Suggest why the resistance of metals increases with temperature.
- 19N.3.hl.TZ0.a(ii): Suggest why the resistance of metals increases with temperature.
- 19N.3.hl.TZ0.4b: State two differences between Type I and Type II superconductors.
- 19N.3.hl.TZ0.4b: State two differences between Type I and Type II superconductors.
- 19N.3.hl.TZ0.b: State two differences between Type I and Type II superconductors.
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19N.3.hl.TZ0.7:
X-ray crystallography of a metal crystal produces a diffraction pattern of bright spots.
Using X-rays of wavelength 1.54 × 10−10 m, the first bright spots were produced at an angle θ of 22.3° from the centre.
Calculate the separation between planes of atoms in the lattice, in meters, using section 1 of the data booklet.
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19N.3.hl.TZ0.7:
X-ray crystallography of a metal crystal produces a diffraction pattern of bright spots.
Using X-rays of wavelength 1.54 × 10−10 m, the first bright spots were produced at an angle θ of 22.3° from the centre.
Calculate the separation between planes of atoms in the lattice, in meters, using section 1 of the data booklet.
- 20N.3.hl.TZ0.4b(i): CNT can act as Type 2 superconductors. Outline why Type 2 superconductors are generally more...
- 20N.3.hl.TZ0.4b(i): CNT can act as Type 2 superconductors. Outline why Type 2 superconductors are generally more...
- 20N.3.hl.TZ0.b(i): CNT can act as Type 2 superconductors. Outline why Type 2 superconductors are generally more...
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20N.3.hl.TZ0.4b(ii):
Explain the role of electrons in superconducting materials in terms of the Bardeen–Cooper–Schrieffer (BCS) theory.
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20N.3.hl.TZ0.4b(ii):
Explain the role of electrons in superconducting materials in terms of the Bardeen–Cooper–Schrieffer (BCS) theory.
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20N.3.hl.TZ0.b(ii):
Explain the role of electrons in superconducting materials in terms of the Bardeen–Cooper–Schrieffer (BCS) theory.