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Date November 2015 Marks available 2 Reference code 15N.3.SL.TZ0.12
Level Standard level Paper Paper 3 Time zone Time zone 0
Command term Show that Question number 12 Adapted from N/A

Question

This question is about relativistic kinematics.

A spacecraft is flying in a straight line above a base station at a speed of 0.8c.

N15/4/PHYSI/SP3/ENG/TZ0/12.b

Suzanne is inside the spacecraft and Juan is on the base station.

[N/A]
[[N/A]]
a.
[N/A]
[[N/A]]
b.i.

While moving away from the base station, Suzanne observes another spacecraft travelling towards her at a speed of 0.8c. Using Galilean transformations, calculate the relative speed of the two spacecraft.

[1]
b.ii.

Using the postulates of special relativity, state and explain why Galilean transformations cannot be used in this case to find the relative speeds of the two spacecraft.

[2]
b.iii.

Using relativistic kinematics, the relative speeds of the two spacecraft is shown to be 0.976c. Suzanne measures the other spacecraft to have a length of 8.00 m. Calculate the proper length of the other spacecraft.

[2]
b.iv.

Suzanne’s spacecraft is on a journey to a star. According to Juan, the distance from the base station to the star is 11.4 ly. Show that Suzanne measures the time taken for her to travel from the base station to the star to be about 9 years.

[2]
c.

Markscheme

[N/A]
a.
[N/A]
b.i.

1.6c;

b.ii.

(one of the) postulates states that the speed of light in a vacuum is the same for all inertial observers;

Galilean transformation will give a relative speed greater than the speed of light;

b.iii.

\(\gamma  = \frac{1}{{\sqrt {1 - {{0.976}^2}} }}{\text{ }}( = 4.59)\);

\({l_0} = (4.56 \times 8.00 = ){\text{ 36.7 (m)}}\);

Note: the final answer for SP3 is different to the HP3.

b.iv.

\(t = \frac{s}{v} = \frac{{11.4}}{{0.8}} = 14.25{\text{ (years)}}\);

\(\Delta {t_0} = \frac{{\Delta t}}{\gamma } = \frac{{14.25}}{{1.67}} = 8.6{\text{ (years)}}\);

Allow ECF from (b).

Accept length contraction with the same result.

c.

Examiners report

Only HL Questions 12(a), (b)(i) and (c) were common with SL questions 12(a), (b)(i) and (c). Many did not address “frame of reference”, only explaining “inertial”. Most could identify the postulate relevant to Galilean transformations but few could earn full marks. The calculation was well done by those who attempted the question.

a.

Only HL Questions 12(a), (b)(i) and (c) were common with SL questions 12(a), (b)(i) and (c). Many did not address “frame of reference”, only explaining “inertial”. Most could identify the postulate relevant to Galilean transformations but few could earn full marks. The calculation was well done by those who attempted the question.

b.i.

Only HL Questions 12(a), (b)(i) and (c) were common with SL questions 12(a), (b)(i) and (c). Many did not address “frame of reference”, only explaining “inertial”. Most could identify the postulate relevant to Galilean transformations but few could earn full marks. The calculation was well done by those who attempted the question.

b.ii.

Only HL Questions 12(a), (b)(i) and (c) were common with SL questions 12(a), (b)(i) and (c). Many did not address “frame of reference”, only explaining “inertial”. Most could identify the postulate relevant to Galilean transformations but few could earn full marks. The calculation was well done by those who attempted the question.

b.iii.

Only HL Questions 12(a), (b)(i) and (c) were common with SL questions 12(a), (b)(i) and (c). Many did not address “frame of reference”, only explaining “inertial”. Most could identify the postulate relevant to Galilean transformations but few could earn full marks. The calculation was well done by those who attempted the question.

b.iv.

Only HL Questions 12(a), (b)(i) and (c) were common with SL questions 12(a), (b)(i) and (c). Many did not address “frame of reference”, only explaining “inertial”. Most could identify the postulate relevant to Galilean transformations but few could earn full marks. The calculation was well done by those who attempted the question.

c.

Syllabus sections

Option A: Relativity » Option A: Relativity (Core topics) » A.1 – The beginnings of relativity

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