vapour pressure
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2022 ◽  
pp. 139354
Author(s):  
Alla P. Toropova ◽  
Andrey A. Toropov ◽  
Alessandra Roncaglioni ◽  
Emilio Benfenati

2021 ◽  
Vol 4 (2) ◽  
pp. 59-64
Author(s):  
Kiagus Ahmad Roni ◽  
Elfidiah Elfidiah ◽  
Tri Amrullah

Pertumbuhan Industri yang saat ini semakin berkembang pesat mengikuti kebutuhan dan permintaan konsumen. Salah satunya adalah kendaraan bermesin yang teknologinya dibuat semakin canggih, berkualitas tinggi dan hemat bahan bakar. Research Octane Number (RON) atau angka oktan riset merupakan angka oktan sebuah bahan bakar untuk mesin menggunakan busi, yang diperoleh dari perbandingan intensitas ketukan dengan campuran bahan bakar acuan ketika keduanya diuji dalam mesin Cooperative Fuel Research (CFR). Nilai RON diambil dengan membandingkan campuran antara iso-Oktana dan n-Heptana. Misalnya, sebuah bahan bakar dengan RON 88 berarti 88% kandungan bahan bakar itu adalah iso-Oktana dan 12%-nya n-Heptana. Pada penelitian ini, proses blending dilakukan dengan cara mencampurkan Premium dengan Octane Booster di Laboratorium R&D di PT. Pertamina RU III Plaju dengan Formulasi Blending Premium RON 88 (995 ml, 990 ml, 985 ml, dan 980 ml) dan Octane Booster (5 ml, 10 ml, 15 ml, dan 20 ml) sehingga menghasilkan Pertalite RON 90 yang berdasarkan pada syarat mutu bahan bakar minyak sesuai Standar Industri Indonesia No. 0258-79. Parameter analisa hasil penelitian adalah Angka Oktan Riset (ASTM D-2699), Specific Grafity (ASTM D-1298), Distilasi (ASTM D-86), dan Reid Vapour Pressure (ASTM D-323) dengan Interprestasi terhadap dosis dan pengaruh terhadap emisi gas buang yang baik.


MAUSAM ◽  
2021 ◽  
Vol 42 (1) ◽  
pp. 77-82
Author(s):  
K. P. KULSHRESTHA ◽  
N. K. BHATIA

Based on 30-year averages of the values of atmospheric pressure, temperature and vapour pressure near the ground surface, value's of radio refractive indices for 18 stations of Rajasthan State and adjoining area near and within international border line, have been computed. Using these data, monthly and annual distributions of radio refractive indices over the area for both morning and evening have been describe-d and discussed which may be useful in radiowave propagation in the area.  


Agronomy ◽  
2021 ◽  
Vol 11 (12) ◽  
pp. 2523
Author(s):  
Jacek Leśny ◽  
Leszek Kuchar ◽  
Monika Panfil ◽  
Dmitri V. Vinogradov ◽  
Ewa Dragańska

This paper presents the methodology of taking measurements of active surface energy balance components using the Bowen method. It discusses the applied measurement system, an important part of which are HMD 50U/50Y measurement sensors from Vaisala, adapted to work in the field. Their operation is a source of data for determining vertical profiles of temperature and water vapour pressure. These data are used to determine the turbulence components of the energy balance, i.e., sensible and latent heat. Measurements taken during the vegetative season on rape field showed that intensive evaporation occurred in the period until the end of June and that its decrease coincided with the decrease in the value of the degree of plant development determined on the basis of LAI records. In spring, during the period of intensive plant development, the decade sums of evaporation reached 30 mm, after which their quantities fell to the range of 10–15 mm. They became higher only in the periods of precipitation, when the water from the interception was available.


2021 ◽  
Author(s):  
Femke A. Jansen ◽  
Remko Uijlenhoet ◽  
Cor M. J. Jacobs ◽  
Adriaan J. Teuling

Abstract. Evaporation forms a large loss term in the water balance of inland water bodies. During summer seasons, which are projected to become warmer with more severe and prolonged periods of drought, the combination of high evaporation rates and increasing demand on freshwater resources forms a challenge for water managers. Correct parameterisation of open water evaporation is crucial to include in operational hydrological models to make well supported predictions of the loss of water through evaporation. Here, we aim to study the controls on open water evaporation of a large lowland reservoir in the Netherlands. To this end, we analyse the dynamics of open water evaporation at two locations, i.e. Stavoren and Trintelhaven, at the border of Lake IJssel (1100 km2) where eddy covariance systems were installed during the summer seasons of 2019 and 2020. From these measurements we find that wind speed and the vertical vapour pressure gradient, but not available energy, can explain most of the variability of observed hourly open water evaporation. This is in agreement with Dalton's model which is a well-established model often used in oceanographic studies for calculating open water evaporation. At the daily timescale, we find that wind speed and water temperature are the main drivers in Stavoren. These observed driving variables of open water evaporation are used to develop simple data-driven models for both measurement locations. Validation of these models demonstrates that a simple model using only two variables, performs well both at the hourly timescale (R2 = 0.84 in Stavoren, and R2 = 0.67 in Trintelhaven), and at the daily timescale (R2 = 0.72 in Stavoren, and R2 = 0.51 in Trintelhaven). Using only routinely measured meteorological variables leads to well performing simple data-driven models at hourly (R2 = 0.78 in Stavoren, and R2 = 0.51 in Trintelhaven) and daily (R2 = 0.85 in Stavoren, and R2 = 0.43 in Trintelhaven) timescales. These results for the summer periods show that global radiation is not directly coupled to open water evaporation at the hourly or even daily timescale, but rather wind speed and vertical gradient of vapour pressure are variables that explain most of the variance of open water evaporation. However, when we extend the time series to a complete year, we find a distinct yearly cycle reflecting the yearly dynamics of global radiation. We find that the commonly used model of Penman (1948) produces results that resemble the yearly cycle of observed evaporation. However, at the diurnal scale estimated evaporation using Penman’s model disagrees with observed evaporation. Therefore, using the Penman equation to model open water evaporation for shorter periods of time is questioned. We would like to stress the importance of including the correct drivers in the parameterization of open water evaporation in hydrological models to adequately represent the role of evaporation in the surface-atmosphere interaction of inland water bodies.


Food Research ◽  
2021 ◽  
Vol 5 (6) ◽  
pp. 109-118
Author(s):  
D. Lentzou ◽  
G. Xanthopoulos ◽  
C. Templalexis ◽  
A. Kaltsa

Transpiration and respiration are two mechanisms of water loss in fresh agricultural products, resulting in visual and texture degradation. Neglecting respiration as a mechanism of water loss may lead to erroneous results at saturation where water vapour pressure deficit is zero and thus water loss is expected to be zero, however, the existence of a finite water loss is noted. In this context, an analysis of the associated with transpiration and respiration water loss in figs (Ficus carica L.) was carried out at 0oC, 10oC and 20oC and 45.64%, 80.22% and 98.65% relative humidity as well as the air conditions of walk-in cold storage rooms. The estimated transpiration rate ranged between 0.11-1.416 mg cm-2 h -1 for a water vapour pressure deficit of 0.0-0.98 kPa. The water vapour pressure deficit estimation was based on the difference between cold air temperature and figs’ surface temperature. The respiration rate was calculated at 0oC, 10oC and 20oC as 0.47±0.08, 0.94±0.11 and 2.69±0.17 mLCO2100g-1 h -1 . Quantification of the water loss showed that at 20oC and saturation, the water loss due to respiration accounts for 3.9% of the respective water loss due to water vapour pressure deficit while on average, the water loss due to respiration accounts for 1.5%, 2.1% and 2.6% of the water loss due to water vapour pressure deficit at 0oC, 10oC and 20oC.


Polymers ◽  
2021 ◽  
Vol 13 (23) ◽  
pp. 4238
Author(s):  
Sudhakara Naidu Neppalli ◽  
Timothy W. Collins ◽  
Zahra Gholamvand ◽  
Cian Cummins ◽  
Michael A. Morris ◽  
...  

We studied the kinetics of swelling in high-χ lamellar-forming poly(styrene)-block- poly(lactic acid) (PS-b-PLA) block copolymer (BCP) by varying the heating rate and monitoring the solvent vapour pressure and the substrate temperature in situ during solvo-thermal vapour annealing (STVA) in an oven, and analysing the resulting morphology. Our results demonstrate that there is not only a solvent vapour pressure threshold (120 kPa), but also that the rate of reaching this pressure threshold has a significant effect on the microphase separation and the resulting morphologies. To study the heating rate effect, identical films were annealed in a tetrahydrofuran (THF) vapour environment under three different ramp regimes, low (rT<1 °C/min), medium (2<rT<3 °C/min) and high (rT>4 °C/min), for 60, 90 and 120 min, respectively, while the solvent vapour pressure and the substrate temperature were measured in real time. The translational order improved significantly with increasing the heating rate. The solvent mass uptake calculated for the different ramp regimes during annealing is linearly proportional to time, indicating that the swelling kinetics followed Case II diffusion. Two stages of the swelling behaviour were observed: (i) diffusion at the initial stages of swelling and (ii) stress relaxation, controlled at later stages. Films with a faster rate of increase in vapour pressure (rP>2 kPa/min) reached the pressure threshold value at an early stage of the swelling and attained a good phase separation. According to our results, highly ordered patterns are only obtained when the volume fraction of the solvent exceeds the polymer volume fraction, i.e., (φs≥φp), during the swelling process, and below this threshold value (φs=0.5), the films did not obtain a good structural order, even at longer annealing times.


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