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Solution
ID: past-exam-of-the-short-options-paper-shared-by-prelims-and-parts-a-and-b-of-the-physics-course-of-the-university-of-oxford/2015/s30/2/1/solution
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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
/
2015
/
S30
/
2
/
1
/
Solution
by
Codex
0
2026-10-25
The source expression
E
=
2
1
μ
v
2
−
GM
m
/
r
is
total
mechanical energy
in the centre-of-
mass
frame, not
kinetic energy
alone. Take
v
0
as
the relative
speed
at
a
large initial separation where the mutual potential is negligible. At closest approach, the radial
relative velocity
is zero, so
conservation of angular momentum
and
conservation of energy
give
μ
b
v
0
=
μ
r
c
v
c
,
2
1
μ
v
0
2
=
2
1
μ
v
c
2
−
r
c
GM
m
.
(1)
Using
M
m
/
μ
=
M
+
m
eliminates
v
c
:
b
2
=
r
c
2
+
v
0
2
2
G
(
M
+
m
)
r
c
.
(2)
An impact occurs when
r
c
≤
R
, where
R
=
r
M
+
r
m
. Since the right side increases with positive
r
c
, the
collision
threshold is
b
col
2
=
R
2
[
1
+
R
v
0
2
2
G
(
M
+
m
)
]
,
f
=
R
v
0
2
2
G
(
M
+
m
)
.
(3)
The mutual
escape velocity
is the relative
speed
at
contact
required to reach infinite separation with zero residual
speed
. Setting total
mechanical energy
to zero gives
v
esc
=
r
M
+
r
m
2
G
(
M
+
m
)
,
f
=
v
esc
2
/
v
0
2
.
(4)
This includes target
recoil
. If the given initial
speed
were instead at
a
finite non-negligible separation, its
potential energy
would have to be retained;
v
0
would then not equal the asymptotic
speed
used in the focusing
formula
.
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:
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