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Past exam of the mathematics course of the University of Cambridge
/
2023
/
ii
/
Paper 1
/
39C
/
b
/
iii
/
Solution
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2023
ii
Paper 1
39C
b
iii
Created
2026-09-24
Updated
2026-09-25
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The
polar shear stress in a Newtonian fluid
is
σ
r
θ
=
μ
[
r
∂
r
∂
(
r
u
θ
)
+
r
1
∂
θ
∂
u
r
]
.
(1)
On
r
=
a
, no slip holds for every
θ
, so
u
θ
=
0
and
∂
θ
u
r
=
0
. Therefore
σ
r
θ
(
a
,
θ
)
=
μ
∂
r
u
θ
(
a
,
θ
)
=
−
μ
ψ
rr
(
a
,
θ
)
.
(2)
Differentiating the solution from part (ii) gives
ψ
rr
(
a
,
θ
)
=
γ
−
2
γ
cos
2
θ
,
(3)
and hence
σ
r
θ
(
a
,
θ
)
=
−
μ
γ
+
2
μ
γ
cos
2
θ
.
(4)
The moment arm and line element are both
a
, so the
torque
exerted by the fluid on the disk per unit axial
length
is
T
z
=
a
2
∫
0
2
π
σ
r
θ
(
a
,
θ
)
d
θ
=
−
2
π
μ
γ
a
2
.
(5)
For
γ
>
0
the negative
sign
denotes the
clockwise
sense
of the ambient shear
rotation
. This agrees with the
hydrodynamic torque on a fixed disk in planar shear
.
Ancestors
(12)
iii
b
39C
Paper 1
ii
2023
Past exam of the mathematics course of the University of Cambridge
Mathematics course of the University of Cambridge
Course of the University of Cambridge
University of Cambridge
List of universities
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