DIAT

Pune, India
Pune, India
SEARCH FILTERS
Time filter
Source Type

News Article | April 28, 2017
Site: marketersmedia.com

— The Global Diamond Wire Market Research Report 2017is a professional and in-depth study on the current state of the Diamond Wire industry. In a word, This report studies Diamond Wire in Global market, especially in North America, Europe, China, Japan, Southeast Asia and India, focuses on top manufacturers in global market, with capacity, production, price, revenue and market share for each manufacturer. Key companies included in this research are Asahi Diamond, Meyer Burger, Noritake, JFS, Nakamura Choukou, Nippon Seisen, Logomatic, Bekaert, ILJIN, READ, A.L.M.T., Saesol, NIABRAZE, MDWEC, DIAT, New Material, Nanjing Sanchao, Zhengzhou Sino-Crystal Diamond and Sunnywell. Market Segment by Region, this report splits Global into several key Region, with sales, revenue, market share and growth rate of Diamond Wire in these regions, from 2011 to 2022 (forecast), like North America, Europe, China, Japan, Southeast Asia and India. Firstly, Diamond Wire Market On the basis of product, this report displays the production, revenue, price, market share and growth rate of each type, primarily split into Long Diamond Saw Wire and Ring Coated Saw Wire. On the basis on the end users/applications, this report focuses on the status and outlook for major applications/end users, consumption (sales) , market share and growth rate of Diamond Wire for each application, including Solar Silicon Cutting, LED Sapphire Cutting, Quartz Cutting and Other. 7 Global Diamond Wire Manufacturers Profiles/Analysis 7.1 Asahi Diamond 7.1.1 Company Basic Information, Manufacturing Base, Sales Area and Its Competitors 7.1.2 Diamond Wire Product Category, Application and Specification 7.1.2.1 Product A 7.1.2.2 Product B 7.1.3 Asahi Diamond Diamond Wire Capacity, Production, Revenue, Price and Gross Margin (2012-2017) 7.1.4 Main Business/Business Overview 7.2 Meyer Burger 7.2.1 Company Basic Information, Manufacturing Base, Sales Area and Its Competitors 7.2.2 Diamond Wire Product Category, Application and Specification 7.2.2.1 Product A 7.2.2.2 Product B 7.2.3 Meyer Burger Diamond Wire Capacity, Production, Revenue, Price and Gross Margin (2012-2017) 7.2.4 Main Business/Business Overview 7.3 Noritake 7.3.1 Company Basic Information, Manufacturing Base, Sales Area and Its Competitors 7.3.2 Diamond Wire Product Category, Application and Specification 7.3.2.1 Product A 7.3.2.2 Product B 7.3.3 Noritake Diamond Wire Capacity, Production, Revenue, Price and Gross Margin (2012-2017) 7.3.4 Main Business/Business Overview Figure Picture of Diamond Wire Figure Global Diamond Wire Production (K Meters) and CAGR (%) Comparison by Types (Product Category) (2012-2022) Figure Global Diamond Wire Production Market Share by Types (Product Category) in 2016 Figure Product Picture of Long Diamond Saw Wire Table Major Manufacturers of Long Diamond Saw Wire Figure Product Picture of Ring Coated Saw Wire Table Major Manufacturers of Ring Coated Saw Wire Figure Global Diamond Wire Consumption (K Meters) by Applications (2012-2022) Figure Global Diamond Wire Consumption Market Share by Applications in 2016 Figure Solar Silicon Cutting Examples Figure LED Sapphire Cutting Examples Figure Quartz Cutting Examples Figure Other Examples Figure Global Diamond Wire Market Size (Million USD) , Comparison (K Meters) and CAGR (%) by Regions (2012-2022) Figure North America Diamond Wire Revenue (Million USD) and Growth Rate (2012-2022) Figure Europe Diamond Wire Revenue (Million USD) and Growth Rate (2012-2022) Figure China Diamond Wire Revenue (Million USD) and Growth Rate (2012-2022) Figure Japan Diamond Wire Revenue (Million USD) and Growth Rate (2012-2022) Figure Southeast Asia Diamond Wire Revenue (Million USD) and Growth Rate (2012-2022) Figure India Diamond Wire Revenue (Million USD) and Growth Rate (2012-2022) Figure Global Diamond Wire Revenue (Million USD) Status and Outlook (2012-2022) Figure Global Diamond Wire Capacity, Production (K Meters) Status and Outlook (2012-2022) Figure Global Diamond Wire Major Players Product Capacity (K Meters) (2012-2017) Table Global Diamond Wire Capacity (K Meters) of Key Manufacturers (2012-2017) Table Global Diamond Wire Capacity Market Share of Key Manufacturers (2012-2017) Figure Global Diamond Wire Capacity (K Meters) of Key Manufacturers in 2016 Figure Global Diamond Wire Capacity (K Meters) of Key Manufacturers in 2017 Figure Global Diamond Wire Major Players Product Production (K Meters) (2012-2017) Table Global Diamond Wire Production (K Meters) of Key Manufacturers (2012-2017) Table Global Diamond Wire Production Share by Manufacturers (2012-2017) Figure 2016 Diamond Wire Production Share by Manufacturers Figure 2017 Diamond Wire Production Share by Manufacturers Figure Global Diamond Wire Major Players Product Revenue (Million USD) (2012-2017) Table Global Diamond Wire Revenue (Million USD) by Manufacturers (2012-2017) Table Global Diamond Wire Revenue Share by Manufacturers (2012-2017) Table 2016 Global Diamond Wire Revenue Share by Manufacturers Table 2017 Global Diamond Wire Revenue Share by Manufacturers Table Global Market Diamond Wire Average Price (USD/Meter) of Key Manufacturers (2012-2017) Figure Global Market Diamond Wire Average Price (USD/Meter) of Key Manufacturers in 2016 Table Manufacturers Diamond Wire Manufacturing Base Distribution and Sales Area For more information, please visit http://www.reportsweb.com/global-diamond-wire-market-research-report-2017


Sakhare D.Y.,University of Pune | Rajkumar,DIAT
International Journal of Engineering and Technology | Year: 2013

As the amount of textual Information increases, we experience a need for Automatic Text Summarizers. In Automatic summarization a text document or a larger corpus of multiple documents are reduced to a short set of words or paragraph that conveys the main meaning of the text. In this paper we proposed various features of Summary extraction. In the proposed approach during training phase, the feature vector is computed for a set of sentences using the feature extraction technique. After that, the feature vector and their corresponding feature scores are used to train the neural network optimally. Later in the testing phase, the input document is subjected to pre-processing and feature extraction techniques. Finally, by making use of sentence score, the most important sentences are extracted from the input document. The experimentation is performed with the DUC 2002 dataset. The features that are to be applied depending upon the size of the Document are also analyzed. The comparative results of the proposed approach and that of MS-Word are also presented here.


Ramchand R.,Indian Institute of Science | Patel C.,Indian Institute of Science | Das A.,Norwegian University of Science and Technology | Sivakumar K.,Indian Institute of Science | And 2 more authors.
IECON Proceedings (Industrial Electronics Conference) | Year: 2010

This paper proposes a simple current error space vector based hysteresis controller for two-level inverter fed Induction Motor (IM) drives. This proposed hysteresis controller retains all advantages of conventional current error space vector based hysteresis controllers like fast dynamic response, simple to implement, adjacent voltage vector switching etc. The additional advantage of this proposed hysteresis controller is that it gives a phase voltage frequency spectrum exactly similar to that of a constant switching frequency space vector pulse width modulated (SVPWM) inverter. In this proposed hysteresis controller the boundary is computed online using estimated stator voltages along alpha and beta axes thus completely eliminating look up tables used for obtaining parabolic hysteresis boundary proposed in [19]. The estimation of stator voltage is carried out using current errors along alpha and beta axes and steady state model of induction motor. The proposed scheme is simple and capable of taking inverter upto six step mode operation, if demanded by drive system. The proposed hysteresis controller based inverter fed drive scheme is simulated extensively using SIMULINK toolbox of MATLAB for steady state and transient performance. The experimental verification for steady state performance of the proposed scheme is carried out on a 3.7kW IM. © 2010 IEEE.


Vinze R.,D.I.A.T. | Chandel S.,D.I.A.T. | Limaye M.D.,R and D E E | Prabhu S.V.,Indian Institute of Technology Bombay
Experimental Thermal and Fluid Science | Year: 2016

Influence of chevron nozzle on local heat transfer distribution over a flat plate impinged by incompressible jets is studied for Reynolds numbers of 28,000, 35,000 and 40,000. Ten different chevron nozzle configurations are studied with a pipe diameter of 10.8 mm. Thin metal foil technique is used with IR camera to measure the wall temperature at nozzle to plate distances (z/d) from 1 to 10. An increase in the local Nusselt number by 26-38% compared to that with circular pipe is measured. It is observed that N10 nozzle (with number of chevron tips n = 8 and chevron tip angle θ = 10°) provides best heat transfer performance. A correlation for the average heat transfer is proposed in present study. A multiplication factor is also introduced to predict local Nusselt number for N10 nozzle. © 2016 Elsevier Inc.


Vinze R.,D.I.A.T. | Chollackal A.,Indian Institute of Technology Bombay | Limaye M.D.,RandDE E | Prabhu S.V.,Indian Institute of Technology Bombay
Experimental Thermal and Fluid Science | Year: 2016

An experimental investigation is carried out to study the local convective heat transfer between smooth wedge shaped plate and a single round underexpanded impinging jet, using thin metal foil technique and IR camera. In the present study experiments are carried out for five different nozzle pressure ratios in the range of 2.36-5.08. The jet-to-wedge apex distance (z/d) is varied from 1 to 12 nozzle diameters. The influence of the included angle of wedge is studied by carrying out experiments for three apex angles of 31.5°, 63° and 94.5°. Heat transfer coefficient is calculated based on wall temperature. The local Nusselt numbers, stagnation point Nusselt numbers and recovery factor distribution are reported in present study. Shadowgraphs are used to explain distribution of Nusselt number and recovery factor. It is concluded that local Nusselt number and recovery factor are greatly affected by the nozzle pressure ratios but independent of wedge apex angle. © 2016 Elsevier Inc.


Hegde C.,RNS Institute of Technology | Prabhu H.R.,Bangalore University | Sagar D.S.,Bangalore University | Shenoy P.D.,Bangalore University | And 2 more authors.
Signal, Image and Video Processing | Year: 2011

Automated security is one of the major concerns of modern times. Secure and reliable authentication systems are in great demand. A biometric trait like the electrocardiogram (ECG) of a person is unique and secure. In this paper, we propose an authentication technique based on Radon transform. Here, ECG wave is considered as an image and Radon transform is applied on this image. Standardized Euclidean distance is applied on the Radon image to get a feature vector. Correlation coefficient between such two feature vectors is computed to authenticate a person. False Acceptance Ratio of the proposed system is found to be 2.19% and False Rejection Ratio is 0.128%. We have developed two more approaches based on statistical features of an ECG wave as our ground work. The result of proposed technique is compared with these two approaches and also with other state-of-the-art alternatives. © 2011 Springer-Verlag London Limited.


Meena H.C.,Indian Institute of Technology Bombay | Reodikar S.A.,Indian Institute of Technology Bombay | Vinze R.,D.I.A.T. | Prabhu S.V.,Indian Institute of Technology Bombay
Experimental Thermal and Fluid Science | Year: 2016

An experimental investigation is performed to study the influence of the shape of the orifice (circular, square, triangular and elliptical), jet to plate distances and Reynolds number on the local heat transfer distribution to normally impinging submerged air jet on smooth and flat surface. The Reynolds numbers were varied from 5000 to 30,000 in the steps of 5000 and the jet to plate distances used were 0.5, 1, 2, 4, 6 and 8. The equivalent diameter (ratio of area to the perimeter) of all the orifices were maintained nearly constant (5.7 mm). The local heat transfer characteristics are estimated using thermal images obtained by infrared thermal imaging technique. For all the shapes, the area averaged Nusselt number increases with increase in Reynolds number. The area averaged Nusselt number at all Reynolds number is observed to be highest at a z/d of 4. Axis switching is observed for all the shapes except circular orifice. The square, triangular and elliptical orifice respectively undergoes a 45°, 180° and 90° axis switch. Pressure loss coefficients of various orifices are reported. © 2015 Elsevier Inc.


Vinze R.,D.I.A.T. | Chandel S.,D.I.A.T. | Limaye M.D.,R and D E E | Prabhu S.V.,Indian Institute of Technology Bombay
Applied Thermal Engineering | Year: 2016

Jet impingement experiments are conducted to study influence of nozzle profile on heat transfer for compressible subsonic jets. Three different circular profiles namely contoured nozzle, orifice and pipe are selected for the present experimental study. For each nozzle profile, Mach numbers covered are 0.3, 0.5 and 0.7 and the corresponding Reynolds numbers are around 48,000, 82,000 and 120,000. Appropriate diameters for these nozzles are chosen to maintain nearly same Reynolds number. Thin metal foil technique with infrared red camera is used to measure the heat transfer coefficient and adiabatic wall temperature. Pressure distribution in the stagnation regions is measured for all the cases. Correlations for local heat transfer distribution over the surface are presented in this study. Pipe nozzle provides higher heat transfer coefficient compared to contoured nozzle and orifice. The Mach number affects the heat transfer in the stagnation region. The recovery factor distribution is insensitive to change in Reynolds number. © 2016 Elsevier Ltd.


Vinze R.,D.I.A.T. | Chandel S.,D.I.A.T. | Limaye M.D.,R and D e E | Prabhu S.V.,Indian Institute of Technology Bombay
International Journal of Thermal Sciences | Year: 2016

Experiments are performed to study the effects of nozzle shape, jet temperature and nozzle to distance (z/de) on heat transfer distribution due to impingement of air jet on a smooth flat plate. Thin metal foil technique is employed in this study for measuring local wall temperature. Influence of jet temperature (70-175 °C) on local heat transfer and effectiveness is studied for different Reynolds numbers (5000-23,000) and jet to plate distances (1-10) for circular jets. Influence of nozzle shape (circular, square and triangular) on local heat transfer distribution and effectiveness is studied for Reynolds number of 10,000 and 23,000 at different jet to plate distances. Reynolds number is calculated on the basis of equivalent diameter (10 mm). Nusselt number measured based on equivalent diameter is the highest for a circular nozzle in comparison with square and triangular nozzles. The effect of jet temperature on heat transfer is found marginal and axis switching is observed for non-circular jets. The axis switching for triangular and square nozzles mechanism is governed by ωx dynamics. © 2015 Elsevier Masson SAS.


Reodikar S.A.,Indian Institute of Technology Bombay | Meena H.C.,Indian Institute of Technology Bombay | Vinze R.,D.I.A.T | Prabhu S.V.,Indian Institute of Technology Bombay
International Journal of Thermal Sciences | Year: 2016

An experimental investigation is performed to study the effects of the orifice shape and Mach number (M) on the local heat transfer distribution by normally impinging compressible jets. Four different orifice cross-sections namely circular, elliptical, square and triangular are used and jets Mach number is maintained from 0.4 to 1in present study. The heat transfer is measured by thin foil IR technique for different nozzle to plate distances. To calculated Nusselt number, adiabatic wall temperature is used as a reference temperature. The stagnation point Nusselt number is significantly higher for circular orifice as compared to other three shapes while that for the elliptical orifice is minimum. Recovery factor distribution is independent of the Reynolds number and the Mach number. The square, triangular and elliptical orifice respectively undergoes a 45°, 180° and 90° axis switching. © 2016 Elsevier Masson SAS. All rights reserved.

Loading DIAT collaborators
Loading DIAT collaborators