User talk:Greg Glover/sandbox
Sandbox
Firearm boox
v2 vg Ek =½mv2
i
=
2
n
{\displaystyle i={\frac {2}{n}}}
{\displaystyle {\sqrt {}}}
n
{\displaystyle {n}}
x
=
−
b
±
b
2
−
4
a
c
2
a
.
{\displaystyle x={\frac {-b\pm {\sqrt {b^{2}-4ac\ }}}{2a}}.}
i
=
2
n
4
n
−
1
n
{\displaystyle i={\frac {2}{n}}{\sqrt {4n-1}}{n}}
i
=
2
n
⋅
4
n
−
1
n
{\displaystyle i={\frac {2}{n}}\cdot {\frac {\sqrt {4n-1}}{n}}}
i
=
2
n
⋅
4
n
−
1
n
{\displaystyle i={\frac {2}{n}}\cdot {\sqrt {\frac {4n-1}{n}}}}
5 Treatment after 5.1 Level of Care
E
k
=
1
2
m
v
2
{\displaystyle E_{k}={\tfrac {1}{2}}mv^{2}}
Kinetic energy
E
t
=
m
v
2
2
g
c
{\displaystyle E_{t}={\tfrac {mv^{2}}{2g_{c}}}}
F
=
m
a
{\displaystyle F=ma\,}
E
0
=
m
c
2
{\displaystyle E_{0}=mc^{2}\,}
E
t
=
w
z
{\displaystyle E_{t}=wz\,}
E
t
=
w
z
{\displaystyle E_{t}=wz}
E
t
=
m
g
v
t
2
g
c
{\displaystyle E_{t}={\tfrac {mgvt}{2g_{c}}}}
E
t
=
m
d
F
t
2
d
t
t
t
2
m
d
t
2
{\displaystyle E_{t}={\tfrac {mdFt^{2}dtt}{t^{2}mdt^{2}}}}
E
t
=
d
F
{\displaystyle E_{t}=dF}
or
E
t
=
f
t
−
l
b
f
{\displaystyle E_{t}=ft-lb_{f}}
g
c
{\displaystyle g_{c}\,}
32.174049
=
m
d
F
t
2
{\displaystyle 32.174049={\tfrac {md}{Ft^{2}}}}
or
32.174049
=
l
b
m
⋅
f
t
l
b
f
⋅
s
2
{\displaystyle 32.174049={\tfrac {lb_{m}\cdot ft}{lb_{f}\cdot s^{2}}}}
or more commonly
32.174 049
32.174049
{\displaystyle 32.174049\,}
E
t
=
.5
⋅
m
v
2
{\displaystyle E_{t}=.5\cdot mv^{2}}
(in SI units of measure in SI mathematical form)
E
t
=
m
v
2
2
{\displaystyle E_{t}={\tfrac {mv^{2}}{2}}}
(in SI units of measure in English Engineering mathematical form)
E
t
=
m
v
2
2
g
c
{\displaystyle E_{t}={\tfrac {mv^{2}}{2g_{c}}}}
(in English Engineering units of measure in English Engineering mathematical form)
h
p
=
f
t
−
l
b
f
⋅
r
p
m
5252
{\displaystyle hp={\tfrac {ft-lb_{f}\cdot rpm}{5252}}}
F
o
r
c
e
(
l
b
f
)
=
m
(
l
b
m
)
⋅
g
(
f
t
/
s
2
)
=
m
(
s
l
u
g
)
⋅
g
(
f
t
/
s
2
)
g
c
(
32.174049
l
b
m
f
t
/
l
b
f
s
e
c
2
)
{\displaystyle Force(lb_{f})=m(lb_{m})\cdot g(ft/s^{2})={\tfrac {m(slug)\cdot g(ft/s^{2})}{g_{c}(32.174049lb_{m}ft/lb_{f}sec^{2})}}}
g
c
=
3.28084
f
t
⋅
2.204623
l
b
m
⋅
4.4482209
l
b
f
{\displaystyle g_{c}=3.28084ft\cdot 2.204623lb_{m}\cdot 4.4482209lb_{f}\,}
-1
⋅
(
s
{\displaystyle \cdot (s\,}
-2
)
=
32.174049
f
t
⋅
l
b
m
⋅
l
b
f
{\displaystyle )=32.174049ft\cdot lb_{m}\cdot lb_{f}\,}
-1
⋅
s
{\displaystyle \cdot s\,}
-2
TKE equations
Substitution: (it yields a totally unrealalistic approximation of free recoil)
E
t
g
u
=
E
t
p
⋅
m
p
m
g
u
⋅
1000
{\displaystyle E_{tgu}=E_{tp}\cdot {\tfrac {m_{p}}{m_{gu}}}\cdot 1000\,}
Short form:
E
t
g
u
=
0.5
⋅
[
(
m
p
⋅
v
p
)
+
(
m
c
⋅
v
c
)
1000
]
2
/
m
g
u
{\displaystyle E_{tgu}=0.5\cdot [{\tfrac {(m_{p}\cdot v_{p})+(m_{c}\cdot v_{c})}{1000}}]^{2}/m_{gu}}
Long form:
v
g
u
=
(
m
p
⋅
v
p
)
+
(
m
c
⋅
v
c
)
1000
/
m
g
u
{\displaystyle v_{gu}={\tfrac {(m_{p}\cdot v_{p})+(m_{c}\cdot v_{c})}{1000}}/m_{gu}}
→
E
t
g
u
=
0.5
⋅
m
g
u
⋅
v
g
u
2
{\displaystyle E_{tgu}=0.5\cdot m_{gu}\cdot v_{gu}^{2}\,}
TKE calculation
E
t
g
u
=
0.5
⋅
[
(
m
p
⋅
v
p
)
+
(
m
c
⋅
v
c
)
1000
]
2
/
m
g
u
{\displaystyle E_{tgu}=0.5\cdot [{\tfrac {(m_{p}\cdot v_{p})+(m_{c}\cdot v_{c})}{1000}}]^{2}/m_{gu}}
and with the numaric values in place;
E
t
g
u
=
0.5
⋅
[
(
9.1
⋅
823
)
+
(
2.75
⋅
1585
)
1000
]
2
/
4.54
=
{\displaystyle E_{tgu}=0.5\cdot [{\tfrac {(9.1\cdot 823)+(2.75\cdot 1585)}{1000}}]^{2}/4.54=}
E
t
g
u
=
0.5
⋅
[
(
7489.3
)
+
(
4358.75
)
1000
]
2
/
4.54
=
{\displaystyle E_{tgu}=0.5\cdot [{\tfrac {(7489.3)+(4358.75)}{1000}}]^{2}/4.54=}
E
t
g
u
=
0.5
⋅
[
11848.05
1000
]
2
/
4.54
=
{\displaystyle E_{tgu}=0.5\cdot [{\tfrac {11848.05}{1000}}]^{2}/4.54=}
E
t
g
u
=
0.5
⋅
11.848
2
/
4.54
=
{\displaystyle E_{tgu}=0.5\cdot 11.848^{2}/4.54=\,}
E
t
g
u
=
0.5
⋅
140.367
/
4.54
=
{\displaystyle E_{tgu}=0.5\cdot 140.367/4.54=\,}
E
t
g
u
=
70.188
/
4.54
=
{\displaystyle E_{tgu}=70.188/4.54=\,}
E
t
g
u
=
15.46
J
=
{\displaystyle E_{tgu}=15.46J=\,}
of free recoil
Torque
τ
=
r
×
F
{\displaystyle {\boldsymbol {\tau }}=\mathbf {r} \times \mathbf {F} \,\!}
τ
=
r
F
sin
θ
{\displaystyle \tau =rF\sin \theta \,\!}
τ
=
r
+
F
{\displaystyle {\boldsymbol {\tau }}=\mathbf {r} +\mathbf {F} \,\!}
τ
=
r
−
F
{\displaystyle {\boldsymbol {\tau }}=\mathbf {r} -\mathbf {F} \,\!}
τ
=
r
×
F
{\displaystyle {\boldsymbol {\tau }}=\mathbf {r} \times \mathbf {F} \,\!}
τ
=
r
⋅
F
{\displaystyle {\boldsymbol {\tau }}=\mathbf {r} \cdot \mathbf {F} \,\!}
τ
=
r
÷
F
{\displaystyle {\boldsymbol {\tau }}=\mathbf {r} \div \mathbf {F} \,\!}
τ
=
r
2
+
F
{\displaystyle {\boldsymbol {\tau }}=\mathbf {r_{2}} +\mathbf {F} \,\!}
τ
=
r
2
+
F
{\displaystyle {\boldsymbol {\tau }}=\mathbf {r^{2}} +\mathbf {F} \,\!}
τ
≡
r
+
F
{\displaystyle {\boldsymbol {\tau }}\equiv \mathbf {r} +\mathbf {F} \,\!}
4
=
2
{\displaystyle {\sqrt {4}}=2}
This is how you strike through.
This is how you Outdent. Every colon (: ) moves the outdent line inboard, one tab.
Pound force
1
l
b
f
{\displaystyle 1lb_{f}\,}
=
1
l
b
m
⋅
g
{\displaystyle =1lb_{m}\cdot g\,}
=
1
l
b
m
⋅
32.174049
f
t
s
2
{\displaystyle ={\tfrac {1lb_{m}\cdot 32.174049ft}{s^{2}}}}
≡
1
k
g
⋅
9.80665
m
s
2
{\displaystyle \equiv {\tfrac {1kg\cdot 9.80665m}{s^{2}}}}
=
4.44822162
N
{\displaystyle =4.44822162N\,}
1 pound-force
= 1 slug·ft/s2
1
l
b
f
{\displaystyle 1lb_{f}\,}
=
1
s
l
u
g
⋅
1
f
t
s
2
{\displaystyle ={\tfrac {1slug\cdot 1ft}{s^{2}}}}
Although force and weight can be mathematically equal, they are two distinct quantities:
F
=
m
a
{\displaystyle F=ma\,}
=
m
d
t
2
{\displaystyle ={\tfrac {md}{t^{2}}}}
and
w
=
m
g
{\displaystyle w=mg\,}
=
m
d
t
2
{\displaystyle ={\tfrac {md}{t^{2}}}}
The use of “mass” as an interchangeable word with “weight” is really an engineering colloquialism. So within the contexts of Newton's Second Law it is incorrect to say weight is equal to mass or to imply that weight is equivalent to mass:
w
=
m
g
≡
m
{\displaystyle w=mg\equiv m}
Frame of reference
Newton's laws of motion for a particle
Euler's laws of motion for rigid bodies and deformable bodies
Rectilinear motion (particle) (kinematics and dynamics)
Curvilinear motion (particle) (Kinematics and dynamics)
Rigid body mechanics (kinematics and dynamics)
Merging Rigid body , Rotational motion
Mention Angular momentum and linking to its main article.
Inertial and non-inertial reference frames formulations.
Centrifugal force
Centripetal force
Coriolis force
That's how you do an Outline
Good afternoon Rracecarr,
would be interested in heading up a “Task force” to clean up and standardize all the pages (stubs) that pertain the Foot-Pound-Second System (FPS). The writings and math for pages like Poundal and Foot-poundal is all over the place. I checked out the Pound (mass) page. What are people thinking and for what reason was the Foot-Pound-Second System page redirected to the Pound (mass) page? See here for the proposal.
I would be more than glad to do as much of the work as possible. I think User:Dorminton and User:MarcusMaximus would support this proposal. Greg Glover (talk ) 20:43, 11 August 2010 (UTC) [ reply ]
Objective: to clean up and standardize pages from the Foot-Pound-Second System, its subsystems and units of measure for writing and math.
Foot-Pound-Second System (FPS)
Redirected the FPS page away from the Pound (mass) page as a new page that will be the main article.
Write and edit new text for this page.
Create subcategory called “Subsystems”
Redirect the English Engineering System page the new FPS page under Subsystems.
Add Gravitational System and Absolute System under Subsystems.
Create a new GravEngAbs box or find the old GravEngAbs box and fix it.
"Pound mass"
Create new page for the pound mass(name to be determined); m = F/a.
Write and edit new text for this page specifying Engineering and Absolute subsystems.
Redirect any references of weight to the Pound (mass) page; F = ma or W = mg/gc.
Pound-foot (torque)
Poundal
Clean up and standardize.
Foot-poundal
Clean up and standardize.
Pound force
Slug
Supported or Unsupported
Use the Foot-pound (energy) page as a template.
Richter magnitude examples (2.0 MJ Base)Table Draft
The following table is the final work as of 2:44pm PDT, 21 MAR 11
Richter magnitudes examples
The following table lists the approximate energy equivalents in terms of TNT explosive force[ 1] – though note that the earthquake energy is released underground rather than overground. Most energy from an earthquake is not transmitted to and through the surface; instead, it dissipates into the crust and other subsurface structures. In contrast, a small atomic bomb blast (see nuclear weapon yield ) will not simply cause light shaking of indoor items, since its energy is released above ground.
As stated above the Richter scale is LOG 10 based. Therefore, the Richter scale numbers may appear grossly understated or or overly stated; 8.1 to 8.12 or 9.0 to 9.02 on this table respectively.
That is because LOG 10 is exponential. Specifically it is exponential between the powers of 0 and 1. 10 to the power of 0 equals 1 and 10 to the power of 1 equals 10.
Following, 31.623 to the power of 0 equals 1, 31.623 to the power of 1 equals 31.623 and 31.623 to the power of 2 equals 1000. Therefore, an 8.0 on the Richter scale releases 31.623 times more energy than a 7.0 and a 9.0 on the Richter scale releases 1000 times more energy than a 7.0.
Richter Approximate Magnitude
Approximate TNT for Seismic Energy Yield
Joule equivalent
Example
0.0
15.0 g
63.1 kJ
0.2
80.3 g (2.83 oz)
337.2 kJ
Large hand grenade
0.5
206.5 g
867.2 kJ
1.0
476.0 g (1.05 lb)
2.0 MJ
Small construction site blast
1.5
6.6 kg
27.6 MJ
2.0
15.0 kg
63.1 MJ
2.5
206.5 kg
867.2 MJ
3.0
476.0 kg
2.0 GJ
3.5
6.6 metric tons
27.6 GJ
3.74
9.5 metric tons
40.0 GJ
Chernobyl nuclear disaster, 1986
3.79
11.0 metric tons
46.2 GJ
Massive Ordnance Air Blast bomb
4.0
15.0 metric tons
63.1 GJ
4.3
118.9 metric tons
499.2 GJ
Kent Earthquake (Britain), 2007
4.5
206.5 metric tons
867.2 GJ
Tajikistan earthquake, 2006
5.0
476.0 kilotons
2.0 TJ
Lincolnshire earthquake (UK), 2008
M
W
{\displaystyle M_{W}}
Ontario-Quebec earthquake (Canada), 2010 [ 2] [ 3]
5.5
6.6 kilotons
27.6 TJ
Little Skull Mtn. earthquake (Nevada, USA), 1992
M
W
{\displaystyle M_{W}}
Alum Rock earthquake (California, USA), 2007
M
W
{\displaystyle M_{W}}
Chino Hills earthquake (Los Angeles, USA), 2008
5.6
8.1 kilotons
34.0 TJ
Newcastle Earthquake Australia, 1989
6.0
15.0 kilotons
63.1 TJ
Double Spring Flat earthquake (Nevada, USA), 1994
6.3
118.9 kilotons
499.2 TJ
M
W
{\displaystyle M_{W}}
Rhodes earthquake (Greece), 2008
Christchurch earthquake (New Zealand), 2011
6.4
161.1 kilotons
676.8 TJ
Kaohsiung earthquake (Taiwan), 2010
6.5
206.5 kilotons
867.2 TJ
M
S
{\displaystyle M_{S}}
Caracas earthquake (Venezuela), 1967
M
W
{\displaystyle M_{W}}
Eureka earthquake (California, USA), 2010
6.6
261.9 kilotons
1.1 PJ
M
W
{\displaystyle M_{W}}
San Fernando earthquake (California, USA), 1971
6.7
309.5 kilotons
1.3 PJ
M
W
{\displaystyle M_{W}}
Northridge earthquake (California, USA), 1994
6.8
357.1 kilotons
1.5 PJ
M
W
{\displaystyle M_{W}}
Nisqually earthquake (Anderson Island, WA), 2001
Gisborne earthquake (Gisborne, NZ), 2007
6.9
404.8 kilotons
1.7 PJ
M
W
{\displaystyle M_{W}}
San Francisco Bay Area earthquake (California, USA), 1989
M
W
{\displaystyle M_{W}}
Pichilemu earthquake (Chile), 2010
7.0
476.0 kilotons
2.0 PJ
M
W
{\displaystyle M_{W}}
Java earthquake (Indonesia), 2009
M
W
{\displaystyle M_{W}}
Haiti earthquake, 2010
7.1
1.5 megatons
6.2 PJ
M
W
{\displaystyle M_{W}}
Messina earthquake (Italy), 1908
M
W
{\displaystyle M_{W}}
San Juan earthquake (Argentina), 1944
M
W
{\displaystyle M_{W}}
Canterbury earthquake (New Zealand), 2010
7.2
2.5 megatons
10.6 PJ
Vrancea earthquake (Romania), 1977
M
W
{\displaystyle M_{W}}
Baja California earthquake (Mexico), 2010
7.5
6.6 megatons
27.6 PJ
M
W
{\displaystyle M_{W}}
Kashmir earthquake (Pakistan), 2005
M
W
{\displaystyle M_{W}}
Antofagasta earthquake (Chile), 2007
7.6
8.1 megatons
34.0 PJ
M
W
{\displaystyle M_{W}}
Gujarat earthquake (India), 2001
7.7
9.7 megatons
40.6 PJ
M
W
{\displaystyle M_{W}}
Sumatra earthquake (Indonesia), 2010
7.8
11.4 megatons
47.8 PJ
M
W
{\displaystyle M_{W}}
Tangshan earthquake (China), 1976
M
S
{\displaystyle M_{S}}
Hawke's Bay earthquake (New Zealand), 1931
M
S
{\displaystyle M_{S}}
Luzon earthquake (Philippines), 1990
8.0
15.0 megatons
63.1 PJ
M
S
{\displaystyle M_{S}}
Mino-Owari earthquake (Japan), 1891
San Juan earthquake (Argentina), 1894
San Francisco earthquake (California, USA), 1906
M
S
{\displaystyle M_{S}}
Queen Charlotte Islands earthquake (B.C., Canada), 1949
M
W
{\displaystyle M_{W}}
Chincha Alta earthquake (Peru), 2007
M
S
{\displaystyle M_{S}}
Sichuan earthquake (China), 2008
8.1
46.2 megatons
194.0 PJ
México City earthquake (Mexico), 1985
Guam earthquake, August 8, 1993[ 4]
8.12
50 megatons
210 PJ
Tsar Bomba - Largest thermonuclear weapon ever tested
8.49
200 megatons
840 PJ
Krakatoa 1883
8.5
206.5 megatons
867.2 PJ
M
W
{\displaystyle M_{W}}
Sumatra earthquake (Indonesia), 2007
8.7
309.5 megatons
1.3 EJ
M
W
{\displaystyle M_{W}}
Sumatra earthquake (Indonesia), 2005
8.8
357.1 megatons
1.5 EJ
M
W
{\displaystyle M_{W}}
Chile earthquake, 2010 ,
9.0
476 gigatons
2.0 EJ
M
W
{\displaystyle M_{W}}
Lisbon earthquake (Portugal), All Saints Day, 1755
M
W
{\displaystyle M_{W}}
Sendai earthquake and tsunami (Japan), 2011
9.02
800 gigatons
3.2 EJ
Toba eruption 75,000 years ago; among the largest known volcanic events.[ 5]
9.2
2.5 gigatons
10.6 EJ
M
W
{\displaystyle M_{W}}
Anchorage earthquake (Alaska, USA), 1964
9.3
3.8 gigatons
15.8 EJ
M
W
{\displaystyle M_{W}}
Sumatra-Andaman earthquake and tsunami (Indonesia), 2004
9.5
6.6 gigatons
27.6 EJ
M
W
{\displaystyle M_{W}}
Valdivia earthquake (Chile), 1960
10.0
15.0 gigatons
63.1 EJ
Never recorded
12.25
95.2 teratons
400 ZJ
Yucatán Peninsula impact (creating Chicxulub crater ) 65 Ma ago (108 megatons; over 4x1030 ergs = 400 ZJ ).[ 6] [ 7] [ 8] [ 9] [ 10]
22.7
309.5×1027 tons
1.3×1039 J
Approximate magnitude of the starquake on the magnetar SGR 1806-20 , registered on December 27, 2004.[ 11]
Good afternoon Glenn L,
As I have stated earlier. I can't do logarithms. I see that you can. As I perceive over the last several months the community has adopted my compromise.
Can you go see here and double check the math?
Richter magnitudes for 2.0 MJ Table Draft
Richter Approximate Magnitude
Approximate TNT for Seismic Energy Yield
Joule equivalent
Example
1.0
476.0 g
2.0 MJ
1.1
1.5 kg
6.2 MJ
1.2
2.5 kg
10.6 MJ
1.3
3.8 kg
15.8 MJ
1.4
5.1 kg
21.4 MJ
1.5
6.6 kg
27.6 MJ
1.6
8.1 kg
34.0 MJ
1.7
9.7 kg
40.6 MJ
1.8
11.4 kg
47.8 MJ
1.9
13.1 kg
55.2 MJ
2.0
15.0 kg
63.1 MJ
2.1
46.2 kg
194.0 MJ
2.2
80.3 kg
337.2 MJ
2.3
118.9 kg
499.2 MJ
2.4
161.1 kg
676.8 MJ
2.5
206.5 kg
867.2 MJ
2.6
261.9 kg
1.1 GJ
2.7
309.5 kg
1.3 GJ
2.8
357.1 kg
1.5 GJ
2.9
404.8 kg
1.7 GJ
3.0
476.0 kg
2.0 GJ
^ FAQs – Measuring Earthquakes
^ "Magnitude 5.0 – Ontario-Quebec border region, Canada" . earthquake.usgs.gov. Retrieved 2010-06-23 .
^ "Moderate 5.0 earthquake shakes Toronto, Eastern Canada and U.S." nationalpost.com. Retrieved 2010-06-23 .
^ "M8.1 South End of Island August 8, 1993" . eeri.org. Retrieved 2011-03-11. .
^ Petraglia, M.; R. Korisettar, N. Boivin, C. Clarkson,4 P. Ditchfield,5 S. Jones,6 J. Koshy,7 M.M. Lahr,8 C. Oppenheimer,9 D. Pyle,10 R. Roberts,11 J.-C. Schwenninger,12 L. Arnold,13 K. White. (6 July 2007). "Middle Paleolithic Assemblages from the Indian Subcontinent Before and After the Toba Super-eruption" . Science 317 (5834): 114–116. doi:10.1126/science.1141564. PMID 17615356.
^ Bralower, Timothy J. (1998). "The Cretaceous-Tertiary boundary cocktail: Chicxulub impact triggers margin collapse and extensive sediment gravity flows" (PDF) . Geology . 26 : 331– 334. doi :10.1130/0091-7613(1998)026<0331:TCTBCC>2.3.CO;2 . ISSN 0091-7613 . Retrieved 2009-09-03 .
^ Klaus, Adam; Norris, Richard D.; Kroon, Dick; Smit, Jan (2000). "Impact-induced mass wasting at the K-T boundary: Blake Nose, western North Atlantic". Geology . 28 : 319– 322. doi :10.1130/0091-7613(2000)28<319:IMWATK>2.0.CO;2 . ISSN 0091-7613 . ;
^ Busby, Cathy J. (2002). "Coastal landsliding and catastrophic sedimentation triggered by Cretaceous-Tertiary bolide impact: A Pacific margin example?". Geology . 30 : 687– 690. doi :10.1130/0091-7613(2002)030<0687:CLACST>2.0.CO;2 . ISSN 0091-7613 . ;
^ Simms, Michael J. (2003). "Uniquely extensive seismite from the latest Triassic of the United Kingdom: Evidence for bolide impact?". Geology . 31 : 557– 560. doi :10.1130/0091-7613(2003)031<0557:UESFTL>2.0.CO;2 . ISSN 0091-7613 .
^ Simkin, Tom (2006). "This dynamic planet. World map of volcanoes, earthquakes, impact craters, and plate tectonics. Inset VI. Impacting extraterrestrials scar planetary surfaces" (PDF) . U.S. Geological Survey. Retrieved 2009-09-03 .
^ Phil Plait (2009). "Anniversary of a cosmic blast" . discovermagazine.com. Retrieved 2010-11-26 .