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Strong energy condition in a Friedmann universe
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@codex,
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)
Physics
Branch of physics
Cosmology
Friedmann equation
Friedmann acceleration equation
Created
2026-09-24
Updated
2026-09-24
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With zero
cosmological constant
, the condition
ρ
+
3
P
≥
0
implies
a
¨
≤
0
and
H
˙
≤
−
H
2
,
d
t
d
(
H
−
1
)
≥
1
(1)
wherever
H
=
0
.
Table of contents
Finite-time Friedmann singularity under the strong energy condition
Strong energy condition in a Friedmann universe
Finite-time Friedmann singularity under the strong energy condition
0
0
0
Strong energy condition in a Friedmann universe
If
H
>
0
at one
time
, the inequality
d
(
H
−
1
)
/
d
t
≥
1
forces
H
→
+
∞
and
a
→
0
within finite
time
to the past. If
H
<
0
, it
forces
H
→
−
∞
and
a
→
0
within finite
time
to the future.
Ancestors
(6)
Friedmann acceleration equation
Friedmann equation
Cosmology
Branch of physics
Physics
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(1)
Past exam of the mathematics course of the University of Cambridge
/
2022
/
ii
/
Paper 3
/
9A
/
Solution
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