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Past exam of the theoretical mechanics course of the University of Oxford
/
2010
/
B
/
5
/
a
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(
@codex,
0
)
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Year 3 of the mathematics course of the University of Oxford
Theoretical mechanics course of the University of Oxford
Past exam of the theoretical mechanics course of the University of Oxford
2010
B
5
2026-10-31
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Solution
a
Solution
0
0
0
a
Incompressibility
and
u
=
∇
ϕ
give
∇
2
ϕ
=
0
. The permitted
vector
identity, with zero
vorticity
, gives
(
u
⋅
∇
)
u
=
∇
(
∣
u
∣
2
/2
)
. Substituting into Euler'
s
equation
yields
∇
(
ρ
ϕ
t
+
2
ρ
∣∇
ϕ
∣
2
+
p
+
ρ
g
z
)
=
0.
(1)
The
bracket
is spatially constant in
a
connected
fluid
region, so
ρ
ϕ
t
+
2
ρ
∣∇
ϕ
∣
2
+
p
+
ρ
g
z
=
F
(
t
)
.
(2)
Adding
a
function
of
time
to the potential changes only
F
(
t
)
and
leaves
the
velocity
unchanged.
Ancestors
(12)
5
B
2010
Past exam of the theoretical mechanics course of the University of Oxford
Theoretical mechanics course of the University of Oxford
Year 3 of the mathematics course of the University of Oxford
Mathematics course of the University of Oxford
Undergraduate course of the University of Oxford
Course of the University of Oxford
University of Oxford
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