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Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
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2018
/
S2
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3
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c
/
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Short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
2018
S2
3
c
2026-10-25
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With zero
curvature
and no
cosmological constant
, the
present
normalization
requires
Ω
M
=
1
. Thus
a
˙
=
H
0
a
−
1/2
, and choosing the
big bang
as
t
=
0
gives
a
(
t
)
=
(
2
3
H
0
t
)
2/3
,
t
0
=
3
H
0
2
.
(1)
For an empty expanding
model
,
Ω
k
=
1
and the
curvature
must be negative. The
equation
becomes
a
˙
=
H
0
,
giving
a
(
t
)
=
H
0
t
,
t
0
=
H
0
−
1
.
(2)
The latter is the Milne slicing of flat
spacetime
; its zero-scale-factor origin is not
a
matter-density
curvature singularity
. In the
matter
model
,
gravity
decelerates expansion, so the earlier
slope
was greater than the
present
slope
and the same
present
size
was reached in less
time
. With the stipulated
H
0
, the two
model
ages are approximately
8.69
and
13.0
Gyr.
Figure 1.
Equal
present
expansion
rates
give different ages when
matter
decelerates expansion
. Both normalized scale factors reach one at the
present
and have the same
slope
there. The
matter
-only
curve
begins two thirds of
a
Hubble time
before the
present
; the empty coasting
curve
begins one
Hubble time
before it.
Details
.
Ancestors
(12)
c
3
S2
2018
Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
Short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
Physics course of the University of Oxford
Undergraduate course of the University of Oxford
Course of the University of Oxford
University of Oxford
List of universities
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