Planet X of mass m1 orbits a Sun in uniform circular motion at a distance r1 and speed v1. The mass of the Sun is MS1 and its radius is RS1 as shown in the figure below.
2) Consider another solar system in which Planet Y of mass m2 = 2 m1 orbits a Sun of mass MS2 = 4 MS1 and radius RS2 = 2RS1 at a distance r2 = 2r1. Further, suppose R2, the radius of Planet Y is twice R1, the radius of Planet X. w2 < w1 w2 = w1 w2 > w1 I think its the last one because the 2's will cancel out but the M2 is 4 so it will be 2 after the canceling. Also how would the speed compare to the original?
@Shadowys Again sorry for the constant badgering. I just want to make certain of my answers.
Nah, it's fine. w being angular velocity?
I think so but it could also be weight.
The previous question asked for speed so it probably be angular velocity.
Yup, if it's angular velocity, then it would be the last one. (I made the assumption that the radius of the planet is very small compared to the suns though)
As did I. Knowing that however, a follow up question asks that how would the velocity compare to the original? v2 = (1/sqrt(2))v1 v2 = (1/2)v1 v2 = v1 v2 = sqrt(2)v1 v2 = 2v1 I think it is the last one because the angular velocity is bigger then w2>w1. All the other options would be less than w1 for example saying that w1=1
Wait. The first is the same. Sorry, I forgot to replace the m2 for the other side. It all cancels out to w1=w2
In thats case, v1=v2 then?
Since w1=w2, subbing \(w=\frac{v}{r}\), we get, \(v_2=2v_1\)
Oh I see. I made a silly assumption of thinking w=v. I have just 1 last question. It involves the springs from an earlier post. Suppose the top (bottom) spring is stretched (compressed) from its relaxed length by an amount δx = 0.082 m. If the spring constant of the top spring is three times that of the bottom spring and M = 0.25 kg and θ = 30o, what is k, the spring constant of the bottom spring? k = 3.73 N/m k = 4.98 N/m k = 6.47 N/m k = 7.47 N/m k = 14.9 N/m I really have no idea on how to start it. I have F = mg(cos30) but not sure on where togo from there.
Well, since it's frictionless, we can skip the y-axis and focus on the x-axis. Since it's not moving, i.e. a=0, taking downwards as positive, and along the incline, \(\Sigma F_x =0\) \(F_gcos 30- (F_{s(top)}+F_{s(bottom)}) =0\) Well, from here sub everything you know in and voila! :) you get k
note: Sorry, it's \(F_gsin 30−(F_{s(top)}+F_{s(bottom)})=0\)
How do I find Top and F bottom respectively?
well, from Hooke's law, \(F_s=kx\), since \(k_{top}\)=3\(k_{bottom}\) and their extensions will be same.
So is the extension .082?
Yup! for both springs.
|dw:1352959869273:dw| I feel like I am doing this wrong
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