Most Used Sayings

Ok, so I'm bored. What is a saying that you frequently use? In example I say, "Navy fucking beans man!" or "Thats Kickass!"

 

"Awesome", "dude", and "that is so cool". My kids all say those too, picked up the habit from hearing me.

 

Aww..thats so cute. My niece runs around giving people the peace sign, saying "Peace man!"

 

That's adorable.

 

"Well... funny story about that"

 

There are lots of phrases that I use frequently. People often tell me I can be quite repetative at times.

There are some that I have trademarked.

For example, I often use the expression "the ________". Another one would be "a __________".

My favorite, though, is "and __________"

I suppose everyone has their own little sayings.

 

thats wicked sick

 

"wicked"
"awwww digga"
"glorious"

 

" who fuckin cares. I don't. go fuck yourself you piece of shit. "

thats even my personal motto.

 

"I'm busy, give me a few minutes and I'll pretend I give a fuck."

 

if i posted them here people would surely get offended.

im not that repetative but ill pull out stupid movies lines and things like that around people who know what im talking bout.

 

nice, i'll add "izzle" before a buncha words, i.e. nizzleice. (izzle + nice) and i say delicious a lot, and lutious. sometimes outta no where i'll just say, "ohhh, no way man!" when nothing at all has happened

 

I have a few of my favorite sayings:

"Right on"

"What the crap?"

"Fantastic"

 

I say "Sweet tits!" when somethng good happens.

 

Folks being offended Here?

Never Thought of that...

 

new one - "wammy"

 

I frequently quote parts of Einsteins Special and General Theory of Relativity. Things like:

"In gravitational fields there are no such things as rigid bodies with Euclidean properties; thus the fictitious rigid body of reference is of no avail in the general theory of relativity. The motion of clocks is also influenced by gravitational fields, and in such a way that a physical definition of time which is made directly with the aid of clocks has by no means the same degree of plausibility as in the special theory of relativity. For this reason non-rigid reference-bodies are used which are as a whole not only moving in any way whatsoever, but which also suffer alterations in form ad lib. during their motion. Clocks, for which the law of motion is any kind, however irregular, serve for the definition of time. We have to imagine each of these clocks fixed at a point on the non-rigid reference-body. These clocks satisfy only the one condition, that the “readings” which are observed simultaneously on adjacent clocks (in space) differ from each other by an indefinitely small amount. This non-rigid reference-body, which might appropriately be termed a “reference-mollusk,” is in the main equivalent to a Gaussian four-dimensional co-ordinate system chosen arbitrarily. That which gives the “mollusk” a certain comprehensibleness as compared with the Gauss co-ordinate system is the (really unqualified) formal retention of the separate existence of the space co-ordinate. Every point on the mollusk is treated as a space-point, and every material point which is at rest relatively to it as at rest, so long as the mollusk is considered as reference-body. The general principle of relativity requires that all these mollusks can be used as reference-bodies with equal right and equal success in the formulation of the general laws of nature; the laws themselves must be quite independent of the choice of mollusk.
We start off from a consideration of a Galileian domain, i.e. a domain in which there is no gravitational field relative to the Galileian reference-body K. The behaviour of measuring-rods and clocks with reference to K is known from the special theory of relativity, likewise the behaviour of “isolated” material points; the latter move uniformly and in straight lines. Now let us refer this domain to a random Gauss co-ordinate system or to a “mollusk” as reference-body K'. Then with respect to K' there is a gravitational field G (of a particular kind). We learn the behaviour of measuring-rods and clocks and also of freely-moving material points with reference to K' simply by mathematical transformation. We interpret this behaviour as the behaviour of measuring-rods, clocks and material points under the influence of the gravitational field G. Hereupon we introduce a hypothesis: that the influence of the gravitational field on measuring-rods, clocks and freely-moving material points continues to take place according to the same laws, even in the case when the prevailing gravitational field is not derivable from the Galileian special case, simply by means of a transformation of co-ordinates. The next step is to investigate the space-time behaviour of the gravitational field G, which was derived from the Galileian special case simply by transformation of the co-ordinates. This behaviour is formulated in a law, which is always valid, no matter how the reference-body (mollusk) used in the description may be chosen."

 

i say 'ridiculous' a lot.
'eh', 'well maybe i should just shut my big mouth', 'i'm an idiot', 'i haven't laughed that hard since i was a little boy', anything with 4 letters...

 

erm, well, I've been calling lots of people "sweetie" "hun" or "dear" lately

 

The Theory of General Relativity is for pussies. Special Relativity, now that's a real mans topic.