Two particles of masses m 1 and m 2 are in the x y plane. The particles are free to move under the influence of their mutual gravitation. At time t = 0 , their positions and velocities are:
( x 1 , y 1 ) = ( 0 , 0 ) ( x 2 , y 2 ) = ( 1 , 0 ) ( x ˙ 1 , y ˙ 1 ) = ( 1 , 0 ) ( x ˙ 2 , y ˙ 2 ) = ( − 0 . 5 , 1 )
Let P 1 = ( x 1 , y 1 ) and P 2 = ( x 2 , y 2 ) be the positions of the particles, and let P be a reference point. Define two displacement vectors:
r 1 = P 1 − P r 2 = P 2 − P
Let the velocities of the particles be v 1 = ( x ˙ 1 , y ˙ 1 ) and v 2 = ( x ˙ 2 , y ˙ 2 ) . The magnitudes of the angular momenta of the particles are:
L 1 = ∣ r 1 × m 1 v 1 ∣ L 2 = ∣ r 2 × m 2 v 2 ∣
The quantity L 1 has a local maximum between t = 0 and t = 1 . What is its value?
Details and Assumptions:
1)
m
1
=
m
2
=
1
2)
Universal gravitational constant
G
=
1
3)
P
=
(
P
x
,
P
y
)
=
(
0
,
3
)
4)
∣
⋅
∣
denotes the magnitude of a vector, and
×
denotes the vector cross product
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@Karan Chatrath Upvoted as always. Can't we solve anaylitcally?
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I did not try solving analytically. I think doing so would be difficult.
@Karan Chatrath Today i have some 2-3 doubts on mechanics. Can you help. Are you free today?
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You could share the problems, and I will try them when I can
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Attached here is a completely numerical solution. Code attached below is commented. I will elaborate on steps further if requested.
Shown below are the plots of the trajectories of the masses and a plot of angular momenta. One can see that the total angular momentum is conserved. This results is expected as no external torque acts on the system.