Re: defining laws in isolation or 'no other force acting'

Gary Oberbrunner <[email protected]> Fri, 31 Jan 2014 06:01:16 -0500
Newsgroups gmane.science.physics.fabric-of-reality
Message-ID <CAFChFyhoUjwyJAag8V6tENcX8HaOufWP2ER4iCRYbYNZrFPUyA@mail.gmail.com>
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On Wed, Jan 22, 2014 at 12:08 AM, <hibbsa-/[email protected]> wrote:

>
>
>
>
> ---In [email protected], <garyo@...> wrote:
>
>
> On Sun, Jan 19, 2014 at 2:26 AM, <hibbsa@...> wrote:
>
>>> the reasoning seems to reverse quite easily, such that the second law
>>> derives from the first.
>>
>>
>> The first law doesn't specify the relationship between force and
>> acceleration (except that there is one). For instance, F=m*a^2 would also
>> lead to bodies at rest staying at rest and bodies in motion staying in that
>> state of motion. (There's no acceleration in either case.) So you can't
>> derive the second law from the first, only the other way.
>>
>> --
>> Gary
>
> You might be tempted to kick yourself when you your brain realizes it's
> true before I can finish writing that "you got the problem right but the
> wrong context" as "F -> a" is the right relationship, but the way it could
> be in terms of "a" is the trivial context, and "m" is the intractable
> problem.
>
> But there's a reason why you couldn't choose "m" even though "F -> a" , is
> literally substituting "m" for "->" (i.e. relationship) in a context that
> you've probably known since you were about 8.
>
> But the intractability of "m" is that in the history of the end to end
> reasoning, "m" never existed, and there was never a way to bring it into
> existence.
>
>
Sorry, I have absolutely no idea what you're talking about here.

-- 
Gary


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      <p>On Wed, Jan 22, 2014 at 12:08 AM, &lt;hibbsa-/[email protected]&gt; wrote:<br>
<br>
&gt;<br>
&gt;<br>
&gt;<br>
&gt;<br>
&gt; ---In [email protected], &lt;garyo@...&gt; wrote:<br>
&gt;<br>
&gt;<br>
&gt; On Sun, Jan 19, 2014 at 2:26 AM, &lt;hibbsa@...&gt; wrote:<br>
&gt;<br>
&gt;&gt;&gt; the reasoning seems to reverse quite easily, such that the second law<br>
&gt;&gt;&gt; derives from the first.<br>
&gt;&gt;<br>
&gt;&gt;<br>
&gt;&gt; The first law doesn&#39;t specify the relationship between force and<br>
&gt;&gt; acceleration (except that there is one). For instance, F=m*a^2 would also<br>
&gt;&gt; lead to bodies at rest staying at rest and bodies in motion staying in that<br>
&gt;&gt; state of motion. (There&#39;s no acceleration in either case.) So you can&#39;t<br>
&gt;&gt; derive the second law from the first, only the other way.<br>
&gt;&gt;<br>
&gt;&gt; --<br>
&gt;&gt; Gary<br>
&gt;<br>
&gt; You might be tempted to kick yourself when you your brain realizes it&#39;s<br>
&gt; true before I can finish writing that &quot;you got the problem right but the<br>
&gt; wrong context&quot; as &quot;F -&gt; a&quot; is the right relationship, but the way it could<br>
&gt; be in terms of &quot;a&quot; is the trivial context, and &quot;m&quot; is the intractable<br>
&gt; problem.<br>
&gt;<br>
&gt; But there&#39;s a reason why you couldn&#39;t choose &quot;m&quot; even though &quot;F -&gt; a&quot; , is<br>
&gt; literally substituting &quot;m&quot; for &quot;-&gt;&quot; (i.e. relationship) in a context that<br>
&gt; you&#39;ve probably known since you were about 8.<br>
&gt;<br>
&gt; But the intractability of &quot;m&quot; is that in the history of the end to end<br>
&gt; reasoning, &quot;m&quot; never existed, and there was never a way to bring it into<br>
&gt; existence.<br>
&gt;<br>
&gt;<br>
Sorry, I have absolutely no idea what you&#39;re talking about here.<br>
<br>
-- <br>
Gary<br>
<br>
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