Namanya Ming Ming, lengkapnya Ming Ming Sari Nuryanti . Memakai gamis hijau, jilbab lebar dan tas ransel berwarna hitam, dia memasuki lobi Universitas Pamulang (UNPAM), Tangerang. Dia adalah mahasiswa semester 1 jurusan akuntansi. Usianya baru 17 tahun. Dan dia adalah salah satu mahasiswa TERPANDAI di kelasnya.Saat kelas usai, dia pergi ke perpus. “Ilmu sangat penting. Dengan Ilmu saya bisa memimpin diri saya. Dengan ilmu saya bisa memimpin keluarga. Dengan ilmu saya bisa memimpin bangsa. Dan dengan ilmu saya bisa memimpin dunia.” Itu asalan Ming Ming kenapa saat istirahat dia lebih senang ke perpustakaan daripada tempat lain. (keren ya…)
Sore hari setelah kuliah usai, Ming Ming menuju salah satu sudut kampus. Di sebuah ruangan kecil, dia bersama beberapa temannya mengadakan pengajian bersama. Ini adalah kegiatan rutin mereka, yang merupakan salah satu unit kegiatan mahasiswa di UNPAM. Setelah itu, dia bergegas keluar dari komplek kampus.
Namun dia tidak naik kendaraan untuk pulang. Sambil berjalan, dia memungut dan mengumpulkan plastik bekas minuman yang dia temui di sepanjang jalan. Dia berjalan kaki sehari kurang lebih 10 km. Selama berjalan itulah, dengan menggunakan karung plastik, dia memperoleh banyak plastik untuk dia bawa pulang.
Rumah Ming Ming jauh dari kampus. Dia tinggal bersama ibu dan 6 orang adiknya yang masih kecil-kecil. Mereka tinggal di sebuah rumah sederhana yang mereka pinjam dari saudara mereka di Kecamatan Rumpin Kabupaten Bogor. Biasanya setelah berjalan hampir 10 km, untuk sampai ke rumahnya Ming Ming menumpang truk. Sopir truk yang lewat, sudah kenal denganya, sehingga mereka selalu memberi tumpangan di bak belakang. Subhanallah, setelah truk berhenti dengan tangkas dia naik ke bak belakang lewat sisi samping yang tinggi itu. (can you imagine it ?)
Ming Ming sekeluarga adalah pemulung. Dia, ibu dan adik-adiknya mengumpulkan plastik, dibersihkan kemudian dijual lagi. Dari memulung sampah inilah mereka hidup dan Ming Ming kuliah.
sumber : http://www.intersat.net.id/forum/index.php?showtopic=229
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If we think of a macroscopic system as consisting of a large number of interacting particles, we know that it has a well defined total energy which satisfies a conservation principle. This simple justification of the existence of a thermodynamic energy function is very different from the historical development because thermodynamics was developed before the atomic theory of matter was well accepted. Historically, the existence of a macroscopic conservation of energy principle was demonstrated by purely macroscopic observations as outlined in the following.
Consider a system enclosed by insulating walls – walls that prevent the system from being heated by the environment. Such a system is thermally isolated. A process in which the state of the system is changed only by work done on the system is called adiabatic. We know from overwhelming empirical evidence that the amount of work needed to change the state of a thermally isolated system depends only on the initial and final states and not on the intermediate states through which the system passes. This independence of the path under these conditions implies that we can define a function E such that for a change from state 1 to state 2, the work done on a thermally isolated system equals the change in E:
W = E2 − E1 = ΔE (adiabatic process)
The quantity E is called the (internal) energy of the system.7 The internal energy is measured with respect to the center of mass.8 The energy E is an example of a state function, that is, it characterizes the state of a macroscopic system and is independent of the path.
Problem
What the difference between the total energy and the internal energy?
If we choose a convenient reference state as the zero of energy, then E has an unique value for each state of the system because W is independent of the path for an adiabatic process. (Remember that in general W depends on the path.)
If we relax the condition that the change be adiabatic and allow the system to interact with its surroundings, we would find in general that ΔE = W. (The difference between ΔE and W is zero for an adiabatic process.) In general, we know that we can increase the energy of a system by doing work on it or by heating it as a consequence of a temperature difference between it and its surroundings. In general, the change in the internal energy of a closed system (fixed number of particles) is given by
ΔE = W + Q (first law of thermodynamics)
The quantity Q is the change in the system’s energy due to heating (Q > 0) or cooling (Q < style=”font-weight: bold;”>Problem
A cylindrical pump contains one mole of a gas. The piston fits tightly so that no air escapes and friction in negligible between the piston and the cylinder walls. The pump is thermally insulated from its surroundings. The piston is quickly pressed inward. What will happen to the temperature of the gas? Explain your reasoning.
So far we have considered two classes of thermodynamic quantities. One class consists of state functions because they have a specific value for each macroscopic state of the system. An example of such a function is the internal energy E. As we have discussed, there are other quantities, such as work and energy transfer due to heating, that do not depend on the state of the system. These latter quantities depend on the thermodynamic process by which the system changed from one state to another.
Originally, many scientists thought that there was a fluid called heat in all substances which could flow from one substance to another. This idea was abandoned many years ago, but is still used in everyday language. Thus, people talk about adding heat to a system. We will avoid this use and whenever possible we will avoid the use of the noun “heat” altogether. Instead, we will refer to a process as heating or cooling if it changes the internal energy of a system without changing any external parameters (such as the external pressure, electric field, magnetic field, etc). Heating occurs whenever two solids at different temperatures are brought into thermal contact. In everyday language we would say that heat flows from the hot to the cold body. However, we prefer to say that energy is transferred from the hotter to the colder body. There is no need to invoke the noun “heat,” and it is misleading to say that heat “flows” from one body to another.
To understand better that there is no such thing as the amount of heat in a body, consider the following simple analogy adapted from Callen A farmer owns a pond, fed by one stream and drained by another. The pond also receives water from rainfall and loses water by evaporation. The pond is the system of interest, the water within it is analogous to the internal energy, the process of transferring water by the streams is analogous to doing work, the process of adding water by rainfall is analogous to heating, and the process of evaporation is analogous to cooling. The only quantity of interest is the water, just as the only quantity of interest is energy in the thermal case. An examination of the change in the amount of water in the pond cannot tell us how the water got there. The terms rain and evaporation refer only to methods of water transfer, just as the terms heating and cooling refer only to methods of energy transfer.
Take a small plastic container and add just enough water to it so that its temperature can be conveniently measured. Then let the water and the bottle come into equilibrium with their surroundings. Measure the temperature of the water, cap the bottle, and shake the bottle until you are too tired to continue further. Then uncap the bottle and measure the water temperature again. If there were a “whole lot of shaking going on,” you would find the temperature had increased a little.
In this example, the temperature of the water increased without heating. We did work on the water, which resulted in an increase in its internal energy as manifested by a rise in the temperature. The same increase in temperature could have been obtained by bringing the water
into contact with a body at a higher temperature. But it would be impossible to determine by making measurements on the water whether shaking or heating had been responsible for taking the system from its initial to its final state. (To silence someone who objects that you heated the
water with “body heat,” wrap the bottle with an insulating material.)
OK, see you again.
source : http://gambutku.com/the-first-law-of-thermodynamics
Consider a system enclosed by insulating walls – walls that prevent the system from being heated by the environment. Such a system is thermally isolated. A process in which the state of the system is changed only by work done on the system is called adiabatic. We know from overwhelming empirical evidence that the amount of work needed to change the state of a thermally isolated system depends only on the initial and final states and not on the intermediate states through which the system passes. This independence of the path under these conditions implies that we can define a function E such that for a change from state 1 to state 2, the work done on a thermally isolated system equals the change in E:
W = E2 − E1 = ΔE (adiabatic process)
The quantity E is called the (internal) energy of the system.7 The internal energy is measured with respect to the center of mass.8 The energy E is an example of a state function, that is, it characterizes the state of a macroscopic system and is independent of the path.
Problem
What the difference between the total energy and the internal energy?
If we choose a convenient reference state as the zero of energy, then E has an unique value for each state of the system because W is independent of the path for an adiabatic process. (Remember that in general W depends on the path.)
If we relax the condition that the change be adiabatic and allow the system to interact with its surroundings, we would find in general that ΔE = W. (The difference between ΔE and W is zero for an adiabatic process.) In general, we know that we can increase the energy of a system by doing work on it or by heating it as a consequence of a temperature difference between it and its surroundings. In general, the change in the internal energy of a closed system (fixed number of particles) is given by
ΔE = W + Q (first law of thermodynamics)
The quantity Q is the change in the system’s energy due to heating (Q > 0) or cooling (Q < style=”font-weight: bold;”>Problem
A cylindrical pump contains one mole of a gas. The piston fits tightly so that no air escapes and friction in negligible between the piston and the cylinder walls. The pump is thermally insulated from its surroundings. The piston is quickly pressed inward. What will happen to the temperature of the gas? Explain your reasoning.
So far we have considered two classes of thermodynamic quantities. One class consists of state functions because they have a specific value for each macroscopic state of the system. An example of such a function is the internal energy E. As we have discussed, there are other quantities, such as work and energy transfer due to heating, that do not depend on the state of the system. These latter quantities depend on the thermodynamic process by which the system changed from one state to another.
Originally, many scientists thought that there was a fluid called heat in all substances which could flow from one substance to another. This idea was abandoned many years ago, but is still used in everyday language. Thus, people talk about adding heat to a system. We will avoid this use and whenever possible we will avoid the use of the noun “heat” altogether. Instead, we will refer to a process as heating or cooling if it changes the internal energy of a system without changing any external parameters (such as the external pressure, electric field, magnetic field, etc). Heating occurs whenever two solids at different temperatures are brought into thermal contact. In everyday language we would say that heat flows from the hot to the cold body. However, we prefer to say that energy is transferred from the hotter to the colder body. There is no need to invoke the noun “heat,” and it is misleading to say that heat “flows” from one body to another.
To understand better that there is no such thing as the amount of heat in a body, consider the following simple analogy adapted from Callen A farmer owns a pond, fed by one stream and drained by another. The pond also receives water from rainfall and loses water by evaporation. The pond is the system of interest, the water within it is analogous to the internal energy, the process of transferring water by the streams is analogous to doing work, the process of adding water by rainfall is analogous to heating, and the process of evaporation is analogous to cooling. The only quantity of interest is the water, just as the only quantity of interest is energy in the thermal case. An examination of the change in the amount of water in the pond cannot tell us how the water got there. The terms rain and evaporation refer only to methods of water transfer, just as the terms heating and cooling refer only to methods of energy transfer.
Take a small plastic container and add just enough water to it so that its temperature can be conveniently measured. Then let the water and the bottle come into equilibrium with their surroundings. Measure the temperature of the water, cap the bottle, and shake the bottle until you are too tired to continue further. Then uncap the bottle and measure the water temperature again. If there were a “whole lot of shaking going on,” you would find the temperature had increased a little.
In this example, the temperature of the water increased without heating. We did work on the water, which resulted in an increase in its internal energy as manifested by a rise in the temperature. The same increase in temperature could have been obtained by bringing the water
into contact with a body at a higher temperature. But it would be impossible to determine by making measurements on the water whether shaking or heating had been responsible for taking the system from its initial to its final state. (To silence someone who objects that you heated the
water with “body heat,” wrap the bottle with an insulating material.)
OK, see you again.
source : http://gambutku.com/the-first-law-of-thermodynamics
Berikut ini adalah daftar nama-nama Kelurahan / Desa dan Kecamatan beserta nomor kode pos (postcode / zip code) pada Kota Palu, Provinsi Sulawesi Tengah (Sulteng), Republik Indonesia.
Negara : Negara Kesatuan Republik Indonesia (NKRI)
Provinsi : Sulawesi Tengah (Sulteng)
Kota Administrasi/Kotamadya : Palu
1. Kecamatan Palu Barat
Daftar nama Desa/Kelurahan di Kecamatan Palu Barat di Kota Palu, Provinsi Sulawesi Tengah (Sulteng) :
- Kelurahan/Desa Baru (Kodepos : 94221)
- Kelurahan/Desa Boyaoge (Kodepos : 94221)
- Kelurahan/Desa Lere (Kodepos : 94221)
- Kelurahan/Desa Siranindi (Kodepos : 94221)
- Kelurahan/Desa Nunu (Kodepos : 94222)
- Kelurahan/Desa Ujuna (Kodepos : 94222)
- Kelurahan/Desa Kamonji (Kodepos : 94223)
- Kelurahan/Desa Duyu (Kodepos : 94225)
- Kelurahan/Desa Balaroa (Kodepos : 94226)
- Kelurahan/Desa Donggala Kodi (Kodepos : 94226)
- Kelurahan/Desa Kabonena (Kodepos : 94227)
- Kelurahan/Desa Silae (Kodepos : 94227)
- Kelurahan/Desa Buluri (Kodepos : 94228)
- Kelurahan/Desa Tipo (Kodepos : 94228)
- Kelurahan/Desa Watusampu (Kodepos : 94229)
2. Kecamatan Palu Selatan
Daftar nama Desa/Kelurahan di Kecamatan Palu Selatan di Kota Palu, Provinsi Sulawesi Tengah (Sulteng) :
- Kelurahan/Desa Birobuli Selatan (Kodepos : 94231)
- Kelurahan/Desa Birobuli Utara (Kodepos : 94231)
- Kelurahan/Desa Petobo (Kodepos : 94232)
- Kelurahan/Desa Kawatuna (Kodepos : 94233)
- Kelurahan/Desa Tanamodindi (Kodepos : 94234)
- Kelurahan/Desa Lolu Selatan (Kodepos : 94235)
- Kelurahan/Desa Lolu Utara (Kodepos : 94235)
- Kelurahan/Desa Tatura Selatan (Kodepos : 94236)
- Kelurahan/Desa Tatura Utara (Kodepos : 94236)
- Kelurahan/Desa Tawanjuka (Kodepos : 94237)
- Kelurahan/Desa Palupi (Kodepos : 94238)
- Kelurahan/Desa Pengawu (Kodepos : 94239)
3. Kecamatan Palu Timur
Daftar nama Desa/Kelurahan di Kecamatan Palu Timur di Kota Palu, Provinsi Sulawesi Tengah (Sulteng) :
- Kelurahan/Desa Besusu Barat (Kodepos : 94111)
- Kelurahan/Desa Besusu Tengah (Kodepos : 94111)
- Kelurahan/Desa Besusu Timur (Kodepos : 94111)
- Kelurahan/Desa Layana Indah (Kodepos : 94111)
- Kelurahan/Desa Poboya (Kodepos : 94115)
- Kelurahan/Desa Lasoani (Kodepos : 94116)
- Kelurahan/Desa Talise (Kodepos : 94118)
- Kelurahan/Desa Tondo (Kodepos : 94119)
4. Kecamatan Palu Utara
Daftar nama Desa/Kelurahan di Kecamatan Palu Utara di Kota Palu, Provinsi Sulawesi Tengah (Sulteng) :
- Kelurahan/Desa Lambara (Kodepos : 94141)
- Kelurahan/Desa Panau (Kodepos : 94141)
- Kelurahan/Desa Baiya (Kodepos : 94142)
- Kelurahan/Desa Pantoloan (Kodepos : 94143)
- Kelurahan/Desa Kayumalue Pajeko (Kodepos : 94145)
- Kelurahan/Desa Kayumalue Ngapa (Kodepos : 94146)
- Kelurahan/Desa Taipa (Kodepos : 94147)
- Kelurahan/Desa Mamboro (Kodepos : 94148)
sumber : http://organisasi.org/daftar-nama-kecamatan-kelurahan-desa-kodepos-di-kota-palu-sulawesi-tengah
Negara : Negara Kesatuan Republik Indonesia (NKRI)
Provinsi : Sulawesi Tengah (Sulteng)
Kota Administrasi/Kotamadya : Palu
1. Kecamatan Palu Barat
Daftar nama Desa/Kelurahan di Kecamatan Palu Barat di Kota Palu, Provinsi Sulawesi Tengah (Sulteng) :
- Kelurahan/Desa Baru (Kodepos : 94221)
- Kelurahan/Desa Boyaoge (Kodepos : 94221)
- Kelurahan/Desa Lere (Kodepos : 94221)
- Kelurahan/Desa Siranindi (Kodepos : 94221)
- Kelurahan/Desa Nunu (Kodepos : 94222)
- Kelurahan/Desa Ujuna (Kodepos : 94222)
- Kelurahan/Desa Kamonji (Kodepos : 94223)
- Kelurahan/Desa Duyu (Kodepos : 94225)
- Kelurahan/Desa Balaroa (Kodepos : 94226)
- Kelurahan/Desa Donggala Kodi (Kodepos : 94226)
- Kelurahan/Desa Kabonena (Kodepos : 94227)
- Kelurahan/Desa Silae (Kodepos : 94227)
- Kelurahan/Desa Buluri (Kodepos : 94228)
- Kelurahan/Desa Tipo (Kodepos : 94228)
- Kelurahan/Desa Watusampu (Kodepos : 94229)
2. Kecamatan Palu Selatan
Daftar nama Desa/Kelurahan di Kecamatan Palu Selatan di Kota Palu, Provinsi Sulawesi Tengah (Sulteng) :
- Kelurahan/Desa Birobuli Selatan (Kodepos : 94231)
- Kelurahan/Desa Birobuli Utara (Kodepos : 94231)
- Kelurahan/Desa Petobo (Kodepos : 94232)
- Kelurahan/Desa Kawatuna (Kodepos : 94233)
- Kelurahan/Desa Tanamodindi (Kodepos : 94234)
- Kelurahan/Desa Lolu Selatan (Kodepos : 94235)
- Kelurahan/Desa Lolu Utara (Kodepos : 94235)
- Kelurahan/Desa Tatura Selatan (Kodepos : 94236)
- Kelurahan/Desa Tatura Utara (Kodepos : 94236)
- Kelurahan/Desa Tawanjuka (Kodepos : 94237)
- Kelurahan/Desa Palupi (Kodepos : 94238)
- Kelurahan/Desa Pengawu (Kodepos : 94239)
3. Kecamatan Palu Timur
Daftar nama Desa/Kelurahan di Kecamatan Palu Timur di Kota Palu, Provinsi Sulawesi Tengah (Sulteng) :
- Kelurahan/Desa Besusu Barat (Kodepos : 94111)
- Kelurahan/Desa Besusu Tengah (Kodepos : 94111)
- Kelurahan/Desa Besusu Timur (Kodepos : 94111)
- Kelurahan/Desa Layana Indah (Kodepos : 94111)
- Kelurahan/Desa Poboya (Kodepos : 94115)
- Kelurahan/Desa Lasoani (Kodepos : 94116)
- Kelurahan/Desa Talise (Kodepos : 94118)
- Kelurahan/Desa Tondo (Kodepos : 94119)
4. Kecamatan Palu Utara
Daftar nama Desa/Kelurahan di Kecamatan Palu Utara di Kota Palu, Provinsi Sulawesi Tengah (Sulteng) :
- Kelurahan/Desa Lambara (Kodepos : 94141)
- Kelurahan/Desa Panau (Kodepos : 94141)
- Kelurahan/Desa Baiya (Kodepos : 94142)
- Kelurahan/Desa Pantoloan (Kodepos : 94143)
- Kelurahan/Desa Kayumalue Pajeko (Kodepos : 94145)
- Kelurahan/Desa Kayumalue Ngapa (Kodepos : 94146)
- Kelurahan/Desa Taipa (Kodepos : 94147)
- Kelurahan/Desa Mamboro (Kodepos : 94148)
sumber : http://organisasi.org/daftar-nama-kecamatan-kelurahan-desa-kodepos-di-kota-palu-sulawesi-tengah
Perdana Menteri Singapur Lee Hsien Loong
Gaji 2,47 Juta USD Per Tahun -> 32,8 Miliar -> 2,7 Miliar Per Bulan
Kepala Pemerintahan Hongkong Donald Tsang Yum-Kuen
Gaji 516.000 USD Pertahun -> 5,9 Miliar -> 494 Juta Per Bulan
Presiden Amerika Barack Obama
Gaji 400.000 USD Pertahun -> 4,6 Miliar -> 383 Juta Perbulan
PM Irlandia Brian Cowen
Gaji USD 341.000 Pertahun -> 3,9 Miliar -> 326 Juta Perbulan
Presiden Prancis Nicholas Sarkozy
Gaji USD 318.000 -> 3,6 Miliar -> 304 Juta Perbula
itulah daftar gaji tertinggi president di dunai.
sekarang kita kembali ke INDONESIA
Dan Gaji PRESIDEN KITA INDONESIA (Bpk SBY) Sebesar
Gaji pokok Rp 30.240.000
Tunjangan jabatan Rp 32.500.000
Total Rp 62.740.000.
Ternyata Isu Yg Selalu Bilang Gaji KETUA KPK Lebih Besar Ternyata Salah..
Karena Gaji KETUA KPK (Bpk ANTASARI AZHAR) Sebesar 62 Juta Pas
Cuma Beda 2 Juta 7 Ratus 40 Ribu
Wakil Presiden:
Gaji Pokok Rp 20.160.000
Tunjangan jabatan Rp 22.000.000
Total Rp 42.160.000
Ketua DPR:
Gaji pokok Rp 5.040.000
Tunjangan jabatan Rp 18.900.000
Uang paket Rp 2.000.000
Komunikasi Intensif Rp 4.968.000
Total Rp 30.908.000
Ketua Mahkamah Agung (MA):
Gaji pokok Rp 5.040.000
Tunjangan jabatan Rp 18.900.000
Uang paket Rp 450.000
Total Rp 24.390.000
sumber : http://www.kaskus.us/showthread.php?t=3409487
Gaji 2,47 Juta USD Per Tahun -> 32,8 Miliar -> 2,7 Miliar Per Bulan
Kepala Pemerintahan Hongkong Donald Tsang Yum-Kuen
Gaji 516.000 USD Pertahun -> 5,9 Miliar -> 494 Juta Per Bulan
Presiden Amerika Barack Obama
Gaji 400.000 USD Pertahun -> 4,6 Miliar -> 383 Juta Perbulan
PM Irlandia Brian Cowen
Gaji USD 341.000 Pertahun -> 3,9 Miliar -> 326 Juta Perbulan
Presiden Prancis Nicholas Sarkozy
Gaji USD 318.000 -> 3,6 Miliar -> 304 Juta Perbula
itulah daftar gaji tertinggi president di dunai.
sekarang kita kembali ke INDONESIA
Dan Gaji PRESIDEN KITA INDONESIA (Bpk SBY) Sebesar
Gaji pokok Rp 30.240.000
Tunjangan jabatan Rp 32.500.000
Total Rp 62.740.000.
Ternyata Isu Yg Selalu Bilang Gaji KETUA KPK Lebih Besar Ternyata Salah..
Karena Gaji KETUA KPK (Bpk ANTASARI AZHAR) Sebesar 62 Juta Pas
Cuma Beda 2 Juta 7 Ratus 40 Ribu
Wakil Presiden:
Gaji Pokok Rp 20.160.000
Tunjangan jabatan Rp 22.000.000
Total Rp 42.160.000
Ketua DPR:
Gaji pokok Rp 5.040.000
Tunjangan jabatan Rp 18.900.000
Uang paket Rp 2.000.000
Komunikasi Intensif Rp 4.968.000
Total Rp 30.908.000
Ketua Mahkamah Agung (MA):
Gaji pokok Rp 5.040.000
Tunjangan jabatan Rp 18.900.000
Uang paket Rp 450.000
Total Rp 24.390.000
sumber : http://www.kaskus.us/showthread.php?t=3409487
Albert Einstein (lahir di Ulm, Kerajaan Württemberg, Kerajaan Jerman, 14 Maret 1879 – meninggal di Princeton, New Jersey, Amerika Serikat, 18 April 1955 pada umur 76 tahun) adalah seorang ilmuwan fisika teoretis yang dipandang luas sebagai ilmuwan terbesar dalam abad ke-20. Dia mengemukakan teori relativitas dan juga banyak menyumbang bagi pengembangan mekanika kuantum, mekanika statistika, dan kosmologi. Dia dianugerahi Penghargaan Nobel dalam Fisika pada tahun 1921 untuk penjelasannya tentang efek fotolistrik dan "pengabdiannya bagi Fisika Teoretis".Setelah teori relativitas umum dirumuskan, Einstein menjadi terkenal ke seluruh dunia, pencapaian yang tidak biasa bagi seorang ilmuwan. Di masa tuanya, keterkenalannya melampaui ketenaran semua ilmuwan dalam sejarah, dan dalam budaya populer, kata Einstein dianggap bersinonim dengan kecerdasan atau bahkan genius. Wajahnya merupakan salah satu yang paling dikenal di seluruh dunia.
sumber : http://id.wikipedia.org/wiki/Albert_Einstein
Ronaldinho (real name: Ronaldo de Assis Moreira, born in Porto Alegre, March 21, 1980; age 31 years) is a Brazilian football player who since July 2008 to defend the team AC Milan. Height is about 180 cm. She earned the world's best player version Fédération Internationale de Football Association in 2004 and 2005.He is a player with the highest incomes exceed the David Beckham of LA Galaxy.
source: http://id.wikipedia.org/wiki/Ronaldinho
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