The daily maximal sensible and latent heat fluxes calculating by BREB were 164.25 W·m-2 and 294.18 W·m-2 , respectively. Energy balance components were as an inverse “U” shape with their diurnal changes.
In this paper,the energy deposition of non-thermal electron beam in tlare loop with a uniform cross-section through the collisional and reverse current processes is calculated,the heating of soft X-ray plasma by non-thermal electron beam and the energy balance in non-thermal flare model are discussed.
Longmen geothermal field reservoir is warm water abundant Middle and Upper Cambrian carbonate rocks,belongs to warm water type hydrothermal reservoir. Warm water recharge is from atmospheric precipitation,during runoff process, water is heating through deep circulation.
A series of free radicals data were tested under thermal simulation at different heating temperatures and times, and quantitative models between free radical concentration(N) of organic matter and time-temperature(TTI) for type I and type II kerogen were obtained.
As applications, the wave equation on?+ × ?+ and the heat equation in a semi-infinite rod are considered in detail.
In a much cited article, Yau  proved that when the Ricci curvature is bounded uniformly below, then the only bounded solution to the heat equation ?tμ=Δμ on [0, ∞) × M which vanishes at t=0 is the one which vanishes evarywhere.
Well-posedness of a semilinear heat equation with weak initial data
In the first part the initial value problem (IVP) of the semilinear heat equation with initial data in is studied.
For the analogs of the heat and wave equation, we give algorithms for approximating the solution, and display the results of implementing these algorithms.
The nonlinear PDEs consist of a heat equation with the Joule heating as a source and a current conservation equation with temperature-dependent electrical conductivity.
In order to get these second-order error estimates, the Joule heating source is used in a changed equivalent form.
There were different TG curves for unprepared and calcined Magnetitum (Cishi) samples on heating.
Compound 3 exhibited the enchased texture of a smectic liquid crystal from 209.4°C to 219.5°C on heating, while 2 exhibited a liquid crystalline phase from 87.4 to 83.2°C on cooling.
In particular, the differential thermal analysis curves for the decomposition of CeO2 nanocrystalline precursor were measured at different heating rates in air by a thermal analyzer (NETZSCH STA 449C, Germany).