Central force
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Central Force. Umiatin,M.Si. The aim : to evaluate characteristic of motion under central force field. A. Introduction. Central Force always directed along the line connecting the center of the two bodies Occurs in : motion of celestial bodies and nuclear interaction.

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Central Force

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Central force

Central Force


Central force

  • The aim : to evaluate characteristic of motion under central force field

A introduction

A. Introduction

  • Central Force always directed along the line connecting the center of the two bodies

  • Occurs in : motion of celestial bodies and nuclear interaction

Central force motion as one body problem

Central Force Motion as One Body Problem

  • Suppose isolated system consist two bodies and separated a distance r = |r| with interaction between them described by a central force F(r), we need six quantities used to describe motion of those particle :

Method 1

Method 1 :

  • To describe those, we need six quantities ( three component of r1 and three component of r2). The equation of motion of those particle are :

  • If F(r) > 0: repusive , F(r) <0 : Attractive. Coupled by :

Method 2

Method 2

  • Describe a system using center mass (R) and relative position (r).

  • R describes the motion of the center of mass and r describes the relative motion of one particle with respect to the other

Central force

No external forces are acting on the system, so the motion of the center of mass is uniform translational motion.

R** = 0.

Central force

  • Where reduced mass define by :

  • Two bodies problem has been simplified into one body problem.

Central force

  • Solve the equation of motion :

  • The center of mass moves with uniform velocity :

  • By choosing the initial condition, vo, to, Ro = 0, the origin of coordinate coincides with center of mass R.

Central force

  • So the position of m1 and m2 which measured from center of mass :

Central force

If m2 >> m1, then reduced mass:

The eq of motion :

Become :

Central force

  • Hence the problem can be treated as a one body problem. Thus, whenever we use mass m instead of µ, we are indicating that the other mass is very large, whereas the use of µindicates that either the two masses are comparable.

B general properties of central force

B. General properties of Central Force

  • Central Force is Confined to a Plane

    If p is the linear momentum of a particle of mass µ, the torque τ about an axis passing through the center of force is :

Central force

  • If the angular momentum L of mass µis constant, its magnitude and direction are fixed in space. Hence, by definition of the cross product, if the direction of L is fixed in space, vectors r and p must lie in a plane perpendicular to L. That is, the motion of particle of mass µ is confined to a plane that is perpendicular to L.

Central force

  • As we the force acting at body is central force, three dimensional problem can be reduced into two dimensional. Using polar coordinate system :

Central force

2. Angular Momentum and Energy are Constant

The angular momentum of a particle of mass µat a distance r from the force center is :

Central force

  • Since there are no dissipative systems and central forces are conservative, the total energy is constant :

3 law of equal areas

3. Law of Equal Areas

Consider a mass µ at a distance r(θ) at time t from the force center O :

Central force

  • Subtituting

C equation of motion

C. Equation of Motion

From the previous description :

  • If we know V(r), these equations can be solved for θ(t) and r(t). The set [θ(t), r(t)] describes the orbit of the particle.

Central force

  • Solve the equation, we find :

  • We will get t(r) then inverse r(t). But we are interested in the equation of the path in term r and θ

Central force

  • We may write :

  • And subtitute :

  • Then :

Suppose the force is f r kr n

Suppose the Force is F(r) = Krn

  • K = constant

  • If n = 1  the solution is motion of harmonic oscillator

  • If n = -2 , eq : coulomb and gravitation force

Other method use lagrangian

Other method : Use Lagrangian

  • Lagrangian of the system :

  • We find

Central force

  • To simplify, use other variable, for example : u in which = 1/r

Central force

  • Next find

  • Therefore :

Central force

  • We can transform into :



1. Find the force law for a central force field that allow a particle to move in logarithmic spiral orbit given by (k and α are constant) :

Central force

  • Solution :

    First determine :

Central force

  • Now determine :

2 find r t and t

2. Find r(t) and θ(t) !

Solution :

3 what is the total energy

3. What is the total energy ?

  • Solution :

Central force

  • We know that

D planetary motion

D. Planetary Motion

The equation for the path of a particle moving under the influence of a central force whose magnitude is inversely proportional to the distance between the particle can be obtain from :

Central force

  • If we define the origin of θ so that the minimum value of r occurs at θ = 0, so

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