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JURNAL PERJALANAN TANJUNG PUTING

JURNAL PERJALANAN TANJUNG PUTING Taman Nasional (TN) Tanjung Puting terletak di semenanjung Kalimantan Tengah. Di sini terdapat konservasi orangutan terbesar di dunia dengan populasi diperkirakan 30.000 sampai 40.000 orangutan yang tersebar di taman nasional dan juga di luar taman nasional ini. Selain itu TN Tanjung Puting juga merupakan cagar biosfer yang ditunjuk pada tahun 1977 dengan area inti TN Tanjung Puting seluas 415.040 ha yang ditetapkan pada tahun 1982. Dengan status TN dan cagar biosfer TN Tanjung Puting ini dapat terjaga kelestariannya dan merupakan daya tarik salah satu wisata di Indonesia. Ini berbeda dengan konservasi orangutan yang terdapat di bagian Kalimantan lainnya di mana kita melihat orangutan di habitat buatan manusia. Oke langsung aja guys saya mau share perjalanan saya tanggal 6 – 8 Februari 2016 ke TNTP. Hari pertama diawali penjemputan dari bandara Iskandar di Pangkalanbun. Pangkalanbun merupakan kota kecil yang memiliki pelabuhan...
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energy equivalency

Laboratory Work Result Wednesday, 28 th April 2010 Thermodynamics and Heat Transfer DETERMINATION OF ENERGY EQUIVALENCY FOR VARIOUS BIOMASS MATERIALS By : Ahmad Eriska Dwi Hutama Putra F14080122 DEPARTMENT OF AGRICULTURAL ENGINEERING FACULTY OF AGRICULTURAL TECHNOLOGY BOGOR AGRICULTURAL UNIVERSITY 2010 INTRODUCTION The energy equivalency of a material, also known calorific value, is the energy that can be released by the material per weight unit if it experiences a complete combustion. The released energy can be transferred to the surroundings measured by various apparatus such as the calorimeter and the Denwar vessel. The calorimeter generally comprises of a smaller vessel inside a large one, so that there is an empty spaces between the two that functions as an isolation for the heat transfer. A type of the calorimeter is the Bomb Calorimeter commonly used for the det...
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heat transfer through plane walls

A. INTRODUCTION A heat transfer situation in which time is not a factor is designed as steady state . The consideration of heat transfer where time is not considered afford some simplification in the analysis. The governing equation for steady state conduction with internal generation is(Welty, 1978 and Holman, 1989) V 2 T + = 0 ………………………………………………………(1) Where : VT : temperature gradient in vector form q : heat flow vector k : thermal conductivity vector which is known as the Poisson equation, and for steady – state conduction without internal generation of heat, the Laplace equation applies : V 2 T = 0 ……………………………………………………………...(2) Both of the above equation apply to an isotropic medium, that is, one whose properties do not vary with direction, physical properties are also presumed independent of temperature. The initial consideration is one – dimensional steady – state conduction without internal ...
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