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Competition and Non-conventional energy:
Competition:
The tariff policy bolsters competition through making it mandatory for a distribution licensee to procure power by competitive bidding through promoting captive power, open access and encouraging multiple players. The policy stipulates in which the Return on Investment should be at par along with other sectors and in which tariffs should be based on norms and achievements. Incentives should be given to motivate investors to be competent.
Non-conventional energy:
The policy promotes non-conventional energy and co-generation sources of energy through specifying a minimum percentage of off take of such energy. The developers of the project are to be provided adequate incentive to avail of the advantages of the Clean Development Mechanism (CDM). The cost of the project will also permit reasonable cost of setting up coal washeries, coal beneficiation system and ash handling and disposal systems.
Q. Use (a) mesh analysis and (b) nodal analysis to determine the voltage ¯V at the terminals A-B of Figure.
Q. Show the schematic arrangement for: (a) one- dimensional addressing, and (b) two-dimensional addressing, if a 32-kbit ROM is used to provide an 8-bit output word.
Questions: a) Give a brief description of the program counter and the data pointer, including their differences. b) Briefly describe what are Byte-Level logical operations
full sub tractor using demultiplexer
Distinguish between paramagnetic and diamagnetic materials, mentioning at least one example of each. Paramagnetic Materials: The atoms of these materials have permanent magne
comment instruction for LIST p=18f4550
For the circuit of Figure(a), obtain the complete solution for the current i L (t) through the 5-H inductor and the voltage v x (t) across the 6- resistor.
Q. The energy stored in a 2-µH inductor is given by w L (t) = 9e -2t µJ for t ≥ 0. Find the inductor current and voltage at t = 1 s.
circuit diagram,working and construction of voltmeter
Q. The full-wave rectified waveform, approximated by the first three terms of its Fourier series, is given by v (ωt) = V m sin (ωt/2), for 0 ≤ ωt ≤ 2π, and where V m = 100
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