Physics 321 Hour 22 Central Force Problems

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Physics 321
Hour 22
Central Force Problems
Straight-line Motion in Spherical or Cylindrical
Coordinates Coordinates
y
r
r
x
a
t
We want to treat r like a Cartesian coordinate, but if we do, if
appears that there’s a force on the mass even when there is
no force!
Understanding the “Fictitious” Force
Think of r like x :
𝐹
0
a
The force acts in the +r direction.
r
Understanding the “Fictitious” Force
π‘₯=π‘Ž
𝑦 = 𝑣𝑑
→ π‘Ÿ=
π‘Ž2 + 𝑣 2 𝑑 2
2𝑣 2 𝑑 𝑣 2 𝑑
π‘Ÿ=
=
2π‘Ÿ
π‘Ÿ
𝑣 2 𝑣 2𝑑 𝑣 2𝑑 𝑣 2
𝑣 2𝑑2
π‘Ÿ=
− 2
=
1− 2
π‘Ÿ
π‘Ÿ π‘Ÿ
π‘Ÿ
π‘Ÿ
𝑣 2 π‘Ÿ2 − 𝑣 2𝑑 2
𝑣 2 π‘Ž2
𝑣 2 π‘Ž2
=
=
= 3
2
2
π‘Ÿ
π‘Ÿ
π‘Ÿ π‘Ÿ
π‘Ÿ
Understanding the “Fictitious” Force
π‘šπ‘£ 2 π‘Ž2
𝐹 = π‘šπ‘Ÿ =
π‘Ÿ3
𝑙 = π‘šπ‘£π‘Ž
𝑙2
𝐹=
π‘šπ‘Ÿ 3
We can define a corresponding potential
energy:
π‘ˆ=−
πΉπ‘‘π‘Ÿ = −
𝑙2
𝑙2
π‘‘π‘Ÿ = +
3
π‘šπ‘Ÿ
2π‘šπ‘Ÿ 2
Before we even consider real forces, we have
to “add” a repulsive centrifugal force or
centrifugal potential to the problem:
𝑙2
𝐹=
π‘šπ‘Ÿ 3
𝑙2
π‘ˆ=+
2π‘šπ‘Ÿ 2
Centrifugal Potential
π‘ˆπ‘π‘’π‘›π‘‘
β„“2
=+
2μπ‘Ÿ 2
π‘ˆπ‘’π‘“π‘“ = π‘ˆπ‘π‘’π‘›π‘‘ + π‘ˆπ‘”
π‘ˆπ‘” = −𝐺
π‘€π‘š
π‘Ÿ
Central Force
• Force is in the radial direction in spherical
coordinates
• The curl is always zero – even if the force isn’t
inverse square
• Source at the origin
𝛼
π›Όπ‘Ÿ
𝐹 = 𝑛 π‘Ÿ = 𝑛+1
π‘Ÿ
π‘Ÿ
• Source at π‘Ÿ1
𝛼(π‘Ÿ2 − π‘Ÿ1 )
𝐹21 =
|π‘Ÿ2 − π‘Ÿ1 |𝑛+1
Central Force
• Source at π‘Ÿ2
𝐹12
• Potential energy
𝛼(π‘Ÿ1 − π‘Ÿ2 )
=
|π‘Ÿ2 − π‘Ÿ1 |𝑛+1
𝛼 𝑛−1
π‘ˆ π‘Ÿ =
,
𝑛−1
π‘Ÿ2 − π‘Ÿ1
𝑛≠1
Inverse-square Force
• Source at π‘Ÿ1
𝐹21
• Potential energy
𝛼(π‘Ÿ2 − π‘Ÿ1 )
=
|π‘Ÿ2 − π‘Ÿ1 |3
𝛼
π‘ˆ π‘Ÿ =
π‘Ÿ2 − π‘Ÿ1
Example
moon_orbit.nb
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