Physics Forums

## Gravitational force on objects

If I take a feather and a rock and drop them at the same time, because of the effect of the gravitational force, we know that the rock will hit the ground first. (The rock experiences a larger gravitational force).

My question is if these objects are dropped at the same time and vertically, then the velocity can be described as $v = gt$, for both objects. Therefore, at $t = 1, v = 9.81 m s^{-1}$ and at $t = 2, v = 19.6 m s^{-1}$. However, i find it difficult to believe the feather will have this velocity. So how does the differences in gravitational force be accounted for in this equation?

Many thanks

PhysOrg.com  physics news on PhysOrg.com  >> Promising doped zirconia>> New X-ray method shows how frog embryos could help thwart disease>> Bringing life into focus

Mentor
Blog Entries: 1

Quote by CAF123 					 				 				If I take a feather and a rock and drop them at the same time, because of the effect of the gravitational force, we know that the rock will hit the ground first. (The rock experiences a larger gravitational force).
The reason that the rock hits first is not because of its greater gravitational force. If only gravity acted, then both would have the same acceleration = g. But other forces are involved, in particular air resistance. Take away the air and the feather and rock will fall together.

I see, many thanks. So essentially the formula only works when considering zero air resistance

## Gravitational force on objects

yes and no...

Just before an object is dropped it has some energy lets call it Estart where

Estart = PEstart + KEstart

Since it's stationary KEstart = 0 so

Estart = PEstart = mgh

When it hits the ground it has some energy, lets call it Eend then

Eend = PEend + KEend

but PEend = 0 so

Eend = KEend = 0.5mv2

If we assume there is no air resistance to be overcome (or any other way for energy to leave the system) then the law of Conservation of Energy says

Estart = Eend

or

mgh = 0.5mv2

Notice how the mass cancels and the velocity of impact is independant of mass

v = SQRT(2gh)

And if it takes $t$ seconds to cover this distance $h$, either $v = gt$ or  $v = \sqrt{2gh}$ can be used to determine this impact velocity, I presume?

Quote by CAF123 					 				 				 $v = \sqrt{2gh}$ can be used to determine this impact velocity, I presume?
That's what i said.

you have two objects of mass M and m, with M>m . if you let them fall, you get from Newton's 2nd law: M a1= - M g m a2= - m g from that you see immediately that a1=a2 which means the speed of the mass M will change by the same ammount in the same time interval as will the speed of mass m.  The mass of the falling object, does not appear in your motion equations. It doesn't affect it. Even if I didn't use the "static model", that the grav force is mg, but used the force: F= G M' m /r  (M':Earth's Mass) the masses of the falling objects would again drop out. Of course that is not obvious, it comes thanks to the equivalence principle, which says that the mass that appears in ma, and the mass that appears in m* (GM'/r) is the same m=m*

Thread Tools

|                                                     |                               |         |
|-----------------------------------------------------|-------------------------------|---------|
| Similar Threads for: Gravitational force on objects |                               |         |
| Thread                                              | Forum                         | Replies |
|                                                     | Classical Physics             | 4       |
|                                                     | Introductory Physics Homework | 2       |
|                                                     | Introductory Physics Homework | 2       |
|                                                     | Introductory Physics Homework | 4       |
|                                                     | Introductory Physics Homework | 6       |
{"extraction_info": {"found_math": true, "script_math_tex": 0, "script_math_asciimath": 0, "math_annotations": 0, "math_alttext": 0, "mathml": 0, "mathjax_tag": 0, "mathjax_inline_tex": 8, "mathjax_display_tex": 0, "mathjax_asciimath": 0, "img_math": 0, "codecogs_latex": 0, "wp_latex": 0, "mimetex.cgi": 0, "/images/math/codecogs": 0, "mathtex.cgi": 0}, "config": {"markdown_headings": true, "markdown_code": true, "boilerplate_config": {"ratio_threshold": 0.18, "absolute_threshold": 20, "end_threshold": 15, "enable": true}, "remove_buttons": true, "remove_image_figures": true, "remove_link_clusters": true, "table_config": {"min_rows": 2, "min_cols": 3, "format": "github"}, "remove_chinese": true, "remove_edit_buttons": true, "extract_latex": true}, "english_confidence": 0.9201180338859558, "perplexity_flag": "middle"}