A particle mass m moves under the attractive force of intensity (ar+b^2)/r^3 per unit mass. How to show that this motion is planar? What does it mean "force of intensity (ar+b^2)/r^3 per unit mass"? The motion is in central field.
torque about origin is zero as it is central motion. So, the direction as well as magnitude of angular momentum will remain constant. Now, \(\overrightarrow{L}=m\overrightarrow{r} \times\overrightarrow{v}\) Now\(\overrightarrow{r}\) is perpendicular to \(\overrightarrow{L}\) and \(\overrightarrow{L}\) is fixed in direction as i said above. This means \(\overrightarrow{r}\) is confined to rotate in the plane perpendicular to \(\overrightarrow{L}\).
Actually, I know how to show that motion in central field is planar. I thought that I have to use a given magnitude of force. Is there a way to show it for this motion under this force?
Well, no matter what is the nature of a central force (attractive, repulsive, inverse squared or whatever), planar motion is its characteristic. Like u can see for this force. It can be written in this vector form. \(\huge{\overrightarrow{F}=-m\frac{(ar+b^{2})\hat{r}}{r^{3}}}\) \(\overrightarrow{\tau}=\overrightarrow{r}\times\overrightarrow{F}\) So, you can see that \(\overrightarrow{\tau}\) will always be zero and then the rest of the reasoning follows.
Also your question is asking the meaning of "force per unit mass" which is clearly acceleration.
I noticed that, in problems, when they say "force of magnitude ______ per mass unit", in Binet's equation there's no m.
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