Temp.
Temperature is the degree of hotness or coldness. Air temperatures are influenced by the local landscape, such as the presence of bodies of water. The air temperature is measured in degrees Celsius and is rounded to the nearest degree. The daytime maximum and nighttime minimum temperatures that a forecaster expects are often expressed as a range. If the forecast issued covers a wide region, the highs and lows are not going to be identical across all areas in that region.
More weather definitions »
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Sun MorningMorning: 6:00 AM - 11:59 AM |
Sun AfternoonAfternoon: 12:00 PM - 5:59 PM |
Sun EveningEvening: 6:00 PM - 11:59 PM |
Sun OvernightOvernight: 12:00 AM - 5:59 AM |
Mon MorningMorning: 6:00 AM - 11:59 AM |
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Temp.
Temperature is the degree of hotness or coldness. Air temperatures are influenced by the local landscape, such as the presence of bodies of water. The air temperature is measured in degrees Celsius and is rounded to the nearest degree. The daytime maximum and nighttime minimum temperatures that a forecaster expects are often expressed as a range. If the forecast issued covers a wide region, the highs and lows are not going to be identical across all areas in that region.
More weather definitions »
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Sun MorningMorning: 6:00 AM - 11:59 AM |
Sun AfternoonAfternoon: 12:00 PM - 5:59 PM |
Sun EveningEvening: 6:00 PM - 11:59 PM |
Sun OvernightOvernight: 12:00 AM - 5:59 AM |
Mon MorningMorning: 6:00 AM - 11:59 AM |
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Temp.
Temperature is the degree of hotness or coldness. Air temperatures are influenced by the local landscape, such as the presence of bodies of water. The air temperature is measured in degrees Celsius and is rounded to the nearest degree. The daytime maximum and nighttime minimum temperatures that a forecaster expects are often expressed as a range. If the forecast issued covers a wide region, the highs and lows are not going to be identical across all areas in that region.
More weather definitions »
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6/
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Sun MorningMorning: 6:00 AM - 11:59 AM |
Sun AfternoonAfternoon: 12:00 PM - 5:59 PM |
Sun EveningEvening: 6:00 PM - 11:59 PM |
Sun OvernightOvernight: 12:00 AM - 5:59 AM |
Mon MorningMorning: 6:00 AM - 11:59 AM |
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Temp.
Temperature is the degree of hotness or coldness. Air temperatures are influenced by the local landscape, such as the presence of bodies of water. The air temperature is measured in degrees Celsius and is rounded to the nearest degree. The daytime maximum and nighttime minimum temperatures that a forecaster expects are often expressed as a range. If the forecast issued covers a wide region, the highs and lows are not going to be identical across all areas in that region.
More weather definitions »
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6°C |
7°C |
6°C |
5°C |
6°C |
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Relative Humidity
Relative humidity is a percentage of water vapour per area at a specific temperature. Relative humidity is calculated at all times of the year, but the humidex is usually only given in the warmer months from May to September.
Relative humidity can be calculated using various methods and instruments. It is a calculation to find out how many grams of water vapour can be held at a given temperature. Usually, the warmer the air, the higher its capacity for holding water vapour. Each specific temperature has a holding limit for water, and the actual amount of water held in the air at the time of measurement can be represented as a percentage.
For example, if a parcel of air at 20ºC has a limit or capacity of 16 grams of water vapour and 16 grams of water vapour is measured, the air's holding capacity is at its maximum and the relative humidity (RH) of the air is said to be 100%. Take the same air with 8 grams of water vapour and your RH is 50%.
More weather definitions »
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93% |
100% |
100% |
93% |
87% |
P.O.P.
P.O.P. stands for "Probability of Precipitation." It does not predict when, where or how much precipitation will occur. When a weather service issues a forecast calling for rain, it is usually followed by a probability.
For example: "P.O.P. 60%." This expression means there is a 60% chance that any random place in the forecast area, such as your home, will receive measurable rainfall. Measurable rainfall means at least 0.2 mm of rain or the water equivalent of snow.
More weather definitions »
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80% |
80% |
80% |
70% |
40% |
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Sun MorningMorning: 6:00 AM - 11:59 AM |
Sun AfternoonAfternoon: 12:00 PM - 5:59 PM |
Sun EveningEvening: 6:00 PM - 11:59 PM |
Sun OvernightOvernight: 12:00 AM - 5:59 AM |
Mon MorningMorning: 6:00 AM - 11:59 AM |
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Temp.
Temperature is the degree of hotness or coldness. Air temperatures are influenced by the local landscape, such as the presence of bodies of water. The air temperature is measured in degrees Celsius and is rounded to the nearest degree. The daytime maximum and nighttime minimum temperatures that a forecaster expects are often expressed as a range. If the forecast issued covers a wide region, the highs and lows are not going to be identical across all areas in that region.
More weather definitions »
|
6°C |
7°C |
6°C |
5°C |
6°C |
|
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Relative Humidity
Relative humidity is a percentage of water vapour per area at a specific temperature. Relative humidity is calculated at all times of the year, but the humidex is usually only given in the warmer months from May to September.
Relative humidity can be calculated using various methods and instruments. It is a calculation to find out how many grams of water vapour can be held at a given temperature. Usually, the warmer the air, the higher its capacity for holding water vapour. Each specific temperature has a holding limit for water, and the actual amount of water held in the air at the time of measurement can be represented as a percentage.
For example, if a parcel of air at 20ºC has a limit or capacity of 16 grams of water vapour and 16 grams of water vapour is measured, the air's holding capacity is at its maximum and the relative humidity (RH) of the air is said to be 100%. Take the same air with 8 grams of water vapour and your RH is 50%.
More weather definitions »
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93% |
100% |
100% |
93% |
87% |
P.O.P.
P.O.P. stands for "Probability of Precipitation." It does not predict when, where or how much precipitation will occur. When a weather service issues a forecast calling for rain, it is usually followed by a probability.
For example: "P.O.P. 60%." This expression means there is a 60% chance that any random place in the forecast area, such as your home, will receive measurable rainfall. Measurable rainfall means at least 0.2 mm of rain or the water equivalent of snow.
More weather definitions »
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80% |
80% |
80% |
70% |
40% |
Rain
Precipitation in the form of liquid water droplets greater than 0.5 mm. If widely scattered, the drop size may be smaller. The intensity of rain is based on rate of fall. "Very light" means that the scattered drops do not completely wet a surface. "Light" means it is greater than a trace and up to 2.5 mm an hour. "Moderate" means the rate of fall is between 2.8 mm to 7.6 mm per hour. "Heavy" means over 7.6 mm per hour.
More weather definitions »
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1-3mm |
1-3mm |
close to 1mm |
less than 1mm |
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Top News Night Sky Note for February 12, 2012
The star Spica is a few degrees above the waning gibbous Moon. Look for the Moon and the star in the southwest at dawn. Saturn is 7 degrees to the upper right of Spica.
Sunrise & Sunset
| Date |
Sunrise |
Sunset |
Length |
Dawn |
Dusk |
Length |
| Feb 12, 2012 |
07:27 |
17:27 |
10:00 |
06:54 |
18:00 |
11:06 |
RMB Exchange Rate
| Currency Name |
Buying Rate |
Cash Buying Rate |
Selling Rate |
Cash Selling Rate |
Middle Rate |
Pub Time |
| GBP |
987.59 |
957.1 |
995.52 |
995.52 |
994.94 |
2012-02-12
00:00:03 |
| HKD |
81.07 |
80.42 |
81.38 |
81.38 |
81.15 |
2012-02-12
00:00:03 |
| USD |
628.61 |
623.57 |
631.13 |
631.13 |
629.37 |
2012-02-12
00:00:03 |
| CHF |
684.01 |
662.9 |
689.51 |
689.51 |
|
2012-02-12
00:00:03 |
| SGD |
497.82 |
482.45 |
501.82 |
501.82 |
|
2012-02-12
00:00:03 |
| SEK |
93.95 |
91.05 |
94.71 |
94.71 |
|
2012-02-12
00:00:03 |
| DKK |
111.24 |
107.8 |
112.13 |
112.13 |
|
2012-02-12
00:00:03 |
| NOK |
109.03 |
105.66 |
109.9 |
109.9 |
|
2012-02-12
00:00:03 |
| JPY |
8.0835 |
7.8339 |
8.1484 |
8.1484 |
8.1026 |
2012-02-12
00:00:03 |
| CAD |
626.13 |
606.8 |
631.16 |
631.16 |
632.15 |
2012-02-12
00:00:03 |
| AUD |
669.21 |
648.55 |
674.58 |
674.58 |
677.11 |
2012-02-12
00:00:03 |
| EUR |
826.74 |
801.21 |
833.38 |
833.38 |
835.9 |
2012-02-12
00:00:03 |
| MOP |
78.76 |
78.1 |
79.06 |
79.06 |
|
2012-02-12
00:00:03 |
| PHP |
14.75 |
14.3 |
14.87 |
14.87 |
|
2012-02-12
00:00:03 |
| THB |
20.37 |
19.74 |
20.53 |
20.53 |
|
2012-02-12
00:00:03 |
| NZD |
519.33 |
|
523.51 |
|
|
2012-02-12
00:00:03 |
| KRW |
|
0.5411 |
|
0.5868 |
|
2012-02-12
00:00:03 |
| RUB |
20.99 |
|
21.15 |
|
|
2012-02-12
00:00:03 |
USD |
628.61 |
623.57 |
631.13 |
631.13 |
629.37 |
2012-02-12
00:00:03 |
CAD |
626.13 |
606.8 |
631.16 |
631.16 |
632.15 |
2012-02-12
00:00:03 |
Physics Paper quantum dot
Arxiv
Feb 10, 2012
PDF Abstract Spin Dependent Thermoelectric Currents of Tunnel Junctions, Small Rings and Quantum Dots: Onsager Theory
K. Bennemann
spin-orbit
Arxiv
Feb 10, 2012
PDF Abstract Fractionalized skyrmion in rotating and rapidly quenched spin-1 Bose-Einstein condensates with spin-orbit coupling
Chao-Fei Liu, Wu-Ming Liu
graphene
Arxiv
Feb 10, 2012
PDF Abstract Negative differential spin conductance in doped zigzag graphene nanoribbons
Ting-Ting Wu, Xue-Feng Wang, Ming-Xing Zhai, Hua Liu, Liping Zhou, Yong-Jin Jiang
Arxiv
Feb 10, 2012
PDF Abstract Electronic band gaps and transport in aperiodic graphene superlattices of Thue-Morse sequence
Tianxing Ma, Chun Liang, Li-Gang Wang, Hai-Qing Lin
Arxiv
Feb 10, 2012
PDF Abstract Graphene radio: Detecting radiowaves with a single atom sheet
Mircea Dragoman, Dan Neculoiu, Alina Cismaru, George Deligeorgis, George Konstantinidis, Daniela Dragoman
Arxiv
Feb 10, 2012
PDF Abstract Study of Thermal Properties of Graphene-Based Structures Using the Force Constant Method
Hossein Karamitaheri, Neophytos Neophytou, Mahdi Pourfath, Hans Kosina
Arxiv
Feb 10, 2012
PDF Abstract Bias-dependent D'yakonov-Perel' spin relaxation in bilayer graphene
Mathias Diez, Guido Burkard
Arxiv
Feb 10, 2012
PDF Abstract Observation of Multiphoton-induced Fluorescence from Nano Graphene Oxide and Its Applications in In vitro and In vivo Bioimaging
Jun Qian, Dan Wang, Li Peng, Wang Xi, Fu-Hong Cai, Zhen-Feng Zhu, Hao He, Ming-Lie Hu, Sailing He
magnetoresistance
Arxiv
Feb 10, 2012
PDF Abstract Observation of Huge Magnetoresistance and Multiferroic-like Behavior of Co Nanoparticles in a C60 matrix
Yutaka Sakai, Eiiti Tamura, Shuhei Toyokawa, Eiji Shikoh, Vlado K. Lazarov, Atsufumi Hirohata, Teruya Shinjo, Yoshishige Suzuki, Masashi Shiraishi
spin
Arxiv
Feb 10, 2012
PDF Abstract Coherent, mechanical control of a single electronic spin
Sungkun Hong, Michael S. Grinolds, Patrick Maletinsky, Ronald L. Walsworth, Mikhail D. Lukin, Amir Yacoby
Arxiv
Feb 10, 2012
PDF Abstract Negative differential spin conductance in doped zigzag graphene nanoribbons
Ting-Ting Wu, Xue-Feng Wang, Ming-Xing Zhai, Hua Liu, Liping Zhou, Yong-Jin Jiang
Arxiv
Feb 10, 2012
PDF Abstract Fractionalized skyrmion in rotating and rapidly quenched spin-1 Bose-Einstein condensates with spin-orbit coupling
Chao-Fei Liu, Wu-Ming Liu
Arxiv
Feb 10, 2012
PDF Abstract Entanglement in a three spin system controlled by electric and magnetic field
Jukub Luczak, Bogdan R. Bulka
Arxiv
Feb 10, 2012
PDF Abstract Electron spin orientation under in-plane optical excitation in GaAs quantum wells
S. Pfalz, R. Winkler, N. Ubbelohde, D. Hägele, M. Oestreich
Arxiv
Feb 10, 2012
PDF Abstract Bias-dependent D'yakonov-Perel' spin relaxation in bilayer graphene
Mathias Diez, Guido Burkard
Arxiv
Feb 10, 2012
PDF Abstract Extended quantum criticality of low-dimensional superconductors near a spin-density-wave instability
A. Sedeki, D. Bergeron, and C. Bourbonnais
Arxiv
Feb 10, 2012
PDF Abstract Critical temperature and correlation length of an elastic interaction model for spin-crossover materials
Taro Nakada, Takashi Mori, Seiji Miyashita, Masamichi Nishino, Synge Todo, William Nicolazzi, Per Arne Rikvold
Arxiv
Feb 10, 2012
PDF Abstract Spin Dependent Thermoelectric Currents of Tunnel Junctions, Small Rings and Quantum Dots: Onsager Theory
K. Bennemann
GaAs
Arxiv
Feb 10, 2012
PDF Abstract Electron spin orientation under in-plane optical excitation in GaAs quantum wells
S. Pfalz, R. Winkler, N. Ubbelohde, D. Hägele, M. Oestreich
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