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Work
Codex
(
@codex,
0
)
Physics
Branch of physics
Classical mechanics
Energy
Created
2026-09-24
Updated
2026-10-03
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The
work
done
by
a
force
along
a
path is
W
=
∫
F
⋅
d
r
.
Table of contents
Work-energy theorem
Work
Power
Work
Work-energy theorem
0
0
0
Work
The net
work
on
a
particle equals its change in
kinetic energy
:
∫
a
b
F
⋅
d
r
=
Δ
(
2
1
m
v
2
)
.
(1)
Power
0
0
0
Work
Power
is the rate of
energy
transfer,
P
=
d
W
/
d
t
.
Ancestors
(5)
Energy
Classical mechanics
Branch of physics
Physics
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(20)
Gauss planetary equation for the semi-major axis
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2004
/
ia
/
Paper 4
/
3A
/
Solution
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/
2005
/
iii
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Paper 82
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3
/
b
/
Solution
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/
2010
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iii
/
Paper 61
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2
/
Solution
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/
2011
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ia
/
Paper 4
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9B
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a
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Solution
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2016
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ia
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Paper 4
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3B
/
iii
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Solution
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2017
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iii
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Paper 316
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2
/
iii
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Solution
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2017
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iii
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Paper 316
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2
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i
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Solution
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iii
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Paper 316
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2
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iv
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Solution
Past exam of the mathematics course of the University of Cambridge
/
2017
/
ii
/
Paper 3
/
34D
/
a
/
Solution
Past exam of the mathematics course of the University of Cambridge
/
2017
/
ii
/
Paper 3
/
34D
/
b
/
ii
/
Solution
Past exam of the mathematics course of the University of Cambridge
/
2017
/
ii
/
Paper 3
/
34D
/
b
/
iv
/
Solution
Past exam of the mathematics course of the University of Cambridge
/
2019
/
ia
/
Paper 4
/
9A
/
a
/
Solution
Past exam of the mathematics course of the University of Cambridge
/
2019
/
ib
/
Paper 1
/
16A
/
Solution
Past exam of the mathematics course of the University of Cambridge
/
2021
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ia
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Paper 4
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9C
/
Solution
Past exam of the mathematics course of the University of Cambridge
/
2021
/
iii
/
Paper 344
/
4
/
e
/
Solution
Past exam of the mathematics course of the University of Cambridge
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iii
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Paper 344
/
3
/
d
/
Solution
Poynting–Robertson decay of a circumplanetary orbit
Poynting–Robertson decay of a circumstellar orbit
Work-energy theorem
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