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when the curve is not simple or linear as diode valve is known as non-ohmic
level curves or contour curvesanother topic that we should look at is that of level curves or also known as contour curves the level curves of the
there are two parts of thermionic emitters-a directly heated emitteri cathode is directly heated by passing currentii thermionic current is lessiii
i the procedure of ejection of electrons from a metal surface by the application of heat is known as thermionic emission and emitted electrons are
it is based on the photovoltaic effect one of the semiconductor regions is made so thin that the light incident on it reaches the p-n junction and
at high reverse voltage due to high electric field the minorities charge carriers while crossing the junction acquires very high velocities a chain
when reverse bias is enhanced the electric field at the junction also enhances at some stage the electric field becomes so high that it breaks the
as electron hole pair because of thermal collisions is continuously formed in the depletion region these are a regular flow of electrons in the
because of concentration difference holes or electron try to vary from their side to other side only these holes or electrons cross the junction
the combustion of propane occurs via the reaction c3h8g5o2g--gt3c02g4h2og hoe many grams of oxygen are required to burn completely 100g of
draw the important resonance contributors for the benzenoium intermediate in the bromination of aniline and explain why ortho para substitution
quadric surfacesearlier we have looked at lines and planes in three dimensions or r3 and when these are used fairly heavily at times in a calculus
scalar equation of planea little more helpful form of the equations is as follows begin with the first form of the vector equation and write a vector
write down the equation of the line which passes through the points 2 -1 3 and 1 4 -3 write all three forms of the equation of the linesolutionto
definition1 given any x1 amp x2 from an interval i with x1 lt x2 if f x1 lt f x2 then f x is increasing on i2
the shape of a graph part i in the earlier section we saw how to employ the derivative to finds out the absolute minimum amp maximum values of a
equations of lines in this part we need to take a view at the equation of a line in r3 as we saw in the earlier section the equation y mxb does
find out the absolute extrema for the given function and interval g t 2t 3 3t 2 -12t 4 on -4 2solution all we actually need to do here is
i it is also known as impure semiconductorii the phenomena of adding impurity is known as
finding absolute extrema of fx on ab0 confirm that the function is continuous on the interval ab1 determine all critical points of fx
a pure semiconductor is known as intrinsic semiconductor it has thermally formed current carriersi they have four electrons in the outer part of
finding absolute extrema now its time to see our first major application of derivatives specified a continuous function fx on an interval ab we
fermats theorem if f x contain a relative extrema at x c amp f prime c exists then x c is a critical point of f x actually it will be a
1 holes works as virtual charge although there is no charge on holes2 effectual volume of hole is more than electron3 mobility of hole is fewer than
the higher power level band is called as the conduction bandi it is also called as empty band of minimum energyii this band is partially filled by