#11
|
|||
|
|||
so, if it takes 1 year to traverse a narrow "wedge" that is 1 million miles
for the sun, it will take 1 year the traverse a wide wedge that is 1/2 million miles from the sun. The "wedges" containing the same area. This is because the gravity is more intense the closer you gat to the sun? Thanks, jojo "G.P" wrote in message .rogers.com... "G.P" wrote in message .rogers.com... "jojo" wrote in message . .. http://home.cvc.org/science/kepler.htm keplers second law ok, I don't get it. can anyone explain this second law in a "dumbed down" way that I might better understand? See those orange "wedges", all of them enclose equal areas, the law states that it takes a planet equal amount of time to sweep across the width of equal area "wedges". That is why in the animation you see that the closer a planet is from the sun the faster it goes (wedges there are shorter that at the opposite end of the orbit). I should have also mentioned that the equal area wedges closer to the sun, since they are shorter they necessarily have to be wider in order to enclose equal area of wedges at the opposite end of the orbit. Therefore, a planet has to sweep a wider wedge width in the same amount of time, consequently the planet has to travel faster. Guillermo |
#12
|
|||
|
|||
"jojo" wrote in message . .. so, if it takes 1 year to traverse a narrow "wedge" that is 1 million miles for the sun, it will take 1 year the traverse a wide wedge that is 1/2 million miles from the sun. The "wedges" containing the same area. This is because the gravity is more intense the closer you gat to the sun?t Right, I am also a newbie on this, but I can tell you there are several ways to look at it: - As per Newton, the gravitational force between 2 objets having masses M and m, separated a distance R, is proportional to the product of their masses and inversaly proportional to the square of the distance R: F = G(Mm/R^2) whre G is the universal constant of gravitation The closer the 2 orbiting "thing" is from the sun the smaller R is and the grater the gravitational force between them. This causes the "thing" to accelerate toward the sun, therefore increasing its speed. - You can see it from the point of view of Conservation of Angular Momentum. A "thing" orbiting the sun has an angular momentum equal to its Mass times its Velocity times the distance from it to the sun (R): Angular Momentum = M x V x R The mass doesn't change. In order for the angular momentum to stay constant when R gets smaller ("thing" getting close to the sun), V has to increase. - Lastly, there is probably an explanation based on the curvature of SpaceTime, I'd love to "hear" such explanation it exist. Guillermo |
#13
|
|||
|
|||
"jojo" wrote in message . .. so, if it takes 1 year to traverse a narrow "wedge" that is 1 million miles for the sun, it will take 1 year the traverse a wide wedge that is 1/2 million miles from the sun. The "wedges" containing the same area. This is because the gravity is more intense the closer you gat to the sun?t Right, I am also a newbie on this, but I can tell you there are several ways to look at it: - As per Newton, the gravitational force between 2 objets having masses M and m, separated a distance R, is proportional to the product of their masses and inversaly proportional to the square of the distance R: F = G(Mm/R^2) whre G is the universal constant of gravitation The closer the 2 orbiting "thing" is from the sun the smaller R is and the grater the gravitational force between them. This causes the "thing" to accelerate toward the sun, therefore increasing its speed. - You can see it from the point of view of Conservation of Angular Momentum. A "thing" orbiting the sun has an angular momentum equal to its Mass times its Velocity times the distance from it to the sun (R): Angular Momentum = M x V x R The mass doesn't change. In order for the angular momentum to stay constant when R gets smaller ("thing" getting close to the sun), V has to increase. - Lastly, there is probably an explanation based on the curvature of SpaceTime, I'd love to "hear" such explanation it exist. Guillermo |
#14
|
|||
|
|||
so...why isn't the orbit circular instead of elliptic?
Once the planet is close pulled close tot he sun, why doesn't it stay close? what force (or lack of force) allows it to move away for the sun in an ellipse? Thanks, jojo "G.P" wrote in message able.rogers.com... "jojo" wrote in message . .. so, if it takes 1 year to traverse a narrow "wedge" that is 1 million miles for the sun, it will take 1 year the traverse a wide wedge that is 1/2 million miles from the sun. The "wedges" containing the same area. This is because the gravity is more intense the closer you gat to the sun?t Right, I am also a newbie on this, but I can tell you there are several ways to look at it: - As per Newton, the gravitational force between 2 objets having masses M and m, separated a distance R, is proportional to the product of their masses and inversaly proportional to the square of the distance R: F = G(Mm/R^2) whre G is the universal constant of gravitation The closer the 2 orbiting "thing" is from the sun the smaller R is and the grater the gravitational force between them. This causes the "thing" to accelerate toward the sun, therefore increasing its speed. - You can see it from the point of view of Conservation of Angular Momentum. A "thing" orbiting the sun has an angular momentum equal to its Mass times its Velocity times the distance from it to the sun (R): Angular Momentum = M x V x R The mass doesn't change. In order for the angular momentum to stay constant when R gets smaller ("thing" getting close to the sun), V has to increase. - Lastly, there is probably an explanation based on the curvature of SpaceTime, I'd love to "hear" such explanation it exist. Guillermo |
#15
|
|||
|
|||
so...why isn't the orbit circular instead of elliptic?
Once the planet is close pulled close tot he sun, why doesn't it stay close? what force (or lack of force) allows it to move away for the sun in an ellipse? Thanks, jojo "G.P" wrote in message able.rogers.com... "jojo" wrote in message . .. so, if it takes 1 year to traverse a narrow "wedge" that is 1 million miles for the sun, it will take 1 year the traverse a wide wedge that is 1/2 million miles from the sun. The "wedges" containing the same area. This is because the gravity is more intense the closer you gat to the sun?t Right, I am also a newbie on this, but I can tell you there are several ways to look at it: - As per Newton, the gravitational force between 2 objets having masses M and m, separated a distance R, is proportional to the product of their masses and inversaly proportional to the square of the distance R: F = G(Mm/R^2) whre G is the universal constant of gravitation The closer the 2 orbiting "thing" is from the sun the smaller R is and the grater the gravitational force between them. This causes the "thing" to accelerate toward the sun, therefore increasing its speed. - You can see it from the point of view of Conservation of Angular Momentum. A "thing" orbiting the sun has an angular momentum equal to its Mass times its Velocity times the distance from it to the sun (R): Angular Momentum = M x V x R The mass doesn't change. In order for the angular momentum to stay constant when R gets smaller ("thing" getting close to the sun), V has to increase. - Lastly, there is probably an explanation based on the curvature of SpaceTime, I'd love to "hear" such explanation it exist. Guillermo |
#16
|
|||
|
|||
"jojo" wrote in message
. .. so...why isn't the orbit circular instead of elliptic? Once the planet is close pulled close tot he sun, why doesn't it stay close? what force (or lack of force) allows it to move away for the sun in an ellipse? Thanks, jojo Don't top post. Energy. Gravity is not an inflexible, inextensible rope. Consider a marble rolling down the inside of a bowl. Why, when the marble gets to the bottom, doesn't it just stop there? |
#17
|
|||
|
|||
"jojo" wrote in message
. .. so...why isn't the orbit circular instead of elliptic? Once the planet is close pulled close tot he sun, why doesn't it stay close? what force (or lack of force) allows it to move away for the sun in an ellipse? Thanks, jojo Don't top post. Energy. Gravity is not an inflexible, inextensible rope. Consider a marble rolling down the inside of a bowl. Why, when the marble gets to the bottom, doesn't it just stop there? |
#18
|
|||
|
|||
"jojo" wrote in message . .. so...why isn't the orbit circular instead of elliptic? Once the planet is close pulled close tot he sun, why doesn't it stay close? what force (or lack of force) allows it to move away for the sun in an ellipse? The answer is inertia/conservation of momentum (Newton's 1st law). Any planet orbiting the sun is continuously falling toward the center of the sun, but the angular momentum causes a motion that is perpendicular to the fall, as a result it moves forward as it moves down, allowing the planet to keep falling toward the sun but also continually missing it. If a planet had a velocity smaller than: V = SQRT((GM)/R) (a) where G is the universal gravitational constant, M is the mass of the sun and R is the radius of the orbit That planet would in fact fall into the sun. If its velocity is exactly as given by formula (a) its orbit would be circular, if its velocity is greater than (a) but smaller than (a) times square root of 2, it would have an elliptical orbit, if its velocity is (a) times square root of 2, or greater, it would have a parabolic orbit (hyperbolic if the velocity is way bigger than (a) times square root of 2), it'd go around the sun just once to never return. BTW, (a) times square root of 2 is known as the escape velocity Corrections welcomed Guillermo |
#19
|
|||
|
|||
"jojo" wrote in message . .. so...why isn't the orbit circular instead of elliptic? Once the planet is close pulled close tot he sun, why doesn't it stay close? what force (or lack of force) allows it to move away for the sun in an ellipse? The answer is inertia/conservation of momentum (Newton's 1st law). Any planet orbiting the sun is continuously falling toward the center of the sun, but the angular momentum causes a motion that is perpendicular to the fall, as a result it moves forward as it moves down, allowing the planet to keep falling toward the sun but also continually missing it. If a planet had a velocity smaller than: V = SQRT((GM)/R) (a) where G is the universal gravitational constant, M is the mass of the sun and R is the radius of the orbit That planet would in fact fall into the sun. If its velocity is exactly as given by formula (a) its orbit would be circular, if its velocity is greater than (a) but smaller than (a) times square root of 2, it would have an elliptical orbit, if its velocity is (a) times square root of 2, or greater, it would have a parabolic orbit (hyperbolic if the velocity is way bigger than (a) times square root of 2), it'd go around the sun just once to never return. BTW, (a) times square root of 2 is known as the escape velocity Corrections welcomed Guillermo |
#20
|
|||
|
|||
"jojo" wrote in message ...
so...why isn't the orbit circular instead of elliptic? Once the planet is close pulled close tot he sun, why doesn't it stay close? what force (or lack of force) allows it to move away for the sun in an ellipse? Momentum. When it's closest to the sun, it's moving too fast for a circular orbit -- that extra velocity (beyond what's needed for a circular orbit at that distance) throws it further out. |
Thread Tools | |
Display Modes | |
|
|
Similar Threads | ||||
Thread | Thread Starter | Forum | Replies | Last Post |
Kepler's second law negates the need for Gravitation | D Bryan | Astronomy Misc | 4 | April 17th 04 06:14 PM |
Kepler's laws and trajectories | tetrahedron | Astronomy Misc | 2 | March 27th 04 05:31 AM |
Kepler's laws | Michael McNeil | Astronomy Misc | 1 | January 23rd 04 04:45 PM |
keplers law | jojo | Misc | 10 | September 15th 03 04:15 AM |