| Class XII |
Physics |
Physics Part-II |
6 |
the depletion region widens due to the change in the electric field. The effective barrier height under reverse bias is (V0+ V ), [Fig. 14.15(b)]. ... |
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| Class XII |
Physics |
Physics Part-II |
6 |
if the forward current exceeds the rated value. The circuit arrangement for studying the V-I characteristics of a diode, (i.e., the variation of cu... |
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| Class XII |
Physics |
Physics Part-II |
6 |
p-n junction diode primerly allows the flow of current only in one direction (forward bias). The forward bias resistance is low as compared to the ... |
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| Class XII |
Physics |
Physics Part-II |
6 |
the transformer. So for a full-wave rectifier the secondary of the transformer is provided with a centre tapping and so it is called centre-tap tra... |
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| Class XII |
Physics |
Physics Part-II |
6 |
a steady value. To get steady dc output from the pulsating voltage normally a capacitor is connected across the output terminals (parallel to the l... |
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| Class XII |
Physics |
Physics Part-II |
6 |
2. Lattice structure and the atomic structure of constituent elements decide whether a particular material will be insulator, metal or semiconducto... |
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| Class XII |
Physics |
Physics Part-II |
6 |
g between the top of valence band (E ) andVthe bottom of the conduction band E . TCe electrons from valence band can be excited by Reprint 2025-26 ... |
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| Class XII |
Physics |
Physics Part-II |
6 |
In compound semiconductors, the change in relative stoichiometric ratio can also change the type of semiconductor. For example, in ideal GaAs the r... |
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| Class XII |
Physics |
Physics Part-II |
6 |
the above. 14.6 In half-wave rectification, what is the output frequency if the input frequency is 50 Hz. What is the output frequency of a full-wa... |
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| Class XII |
Physics |
Physics Part-I |
7 |
Chapter Seven ALTERNATING CURRENT 7.1 I NTRODUCTION sources. These currents do not change direction with time. But voltages dc and currents that va... |
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| Class XII |
Physics |
Physics Part-I |
7 |
andω is its angular frequency. Nicola Tesla (1856 – 1943) Serbian-American ) scientist, inventor and 3 genius. He conceived the 9 idea of the rotat... |
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| Class XII |
Physics |
Physics Part-I |
7 |
during each cycle. Thus, the sum of the instantaneous current values over one complete cycle is zero, and the average current 178 is zero. The fact... |
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| Class XII |
Physics |
Physics Part-I |
7 |
as dc power and enlisted the services ( (P = I R), a special value of current is defined and used. of Nicola Tesla and 8 It is called, root mean sq... |
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| Class XII |
Physics |
Physics Part-I |
7 |
rms value with a peak voltage of vm= 2 V = (1.414)(220 V) = 311 V In fact, the I or rms current is the equivalent dc current that would produce the... |
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| Class XII |
Physics |
Physics Part-I |
7 |
I represent the amplitudes or the peak values vmand i mf these oscillating quantities. Figure 7.4(a) shows the FIGURE 7.4 (a) A phasor diagram for ... |
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| Class XII |
Physics |
Physics Part-I |
7 |
corresponding magnitudes and directions. The rotating vectors that represent harmonically varying scalar quantities are introduced only to provide ... |
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| Class XII |
Physics |
Physics Part-I |
7 |
t a m The amplitude of the current is, then i n a . im = v m e w X L (7.14) t w r : The dimension of inductive reactance is the same as that of res... |
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| Class XII |
Physics |
Physics Part-I |
7 |
ωt) So, the average power over a complete cycle is P = − m vm sin(2ω t) L 2 i v = − m m sin(2ω t) = 0, since the average of sin (2 t) over a comple... |
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| Class XII |
Physics |
Physics Part-I |
7 |
time t. The instantaneous voltage v across the capacitor is q v = (7.15) C From the Kirchhoff’s loop rule, the voltage across the source and the ca... |
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| Class XII |
Physics |
Physics Part-I |
7 |
to the capacitor is pc= i v =m cos(ω t)m sin(ωt) = m m cos( ωt) sinωt) =im m sin(2ωt) 2 (7.19) So, as in the case of an inductor, the average power... |
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| Class XII |
Physics |
Physics Part-I |
7 |
A) =1.47A E This current oscillates between +1.47A and –1.47 A, and is ahead of P the voltage by p/2. M X If the frequency is doubled, the capaciti... |
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| Class XII |
Physics |
Physics Part-I |
7 |
method, we solve connected to an ac source. Eq. (7.20) analytically to obtain the time– 186 dependence of i. Reprint 2026-27 Alternating Current 7.... |
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| Class XII |
Physics |
Physics Part-I |
7 |
magnitude ‰v Cm – v Lm Since V is represented as the hypotenuse of a right-triangle whose sides are V and (R + V ), Che L pythagorean theorem gives... |
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| Class XII |
Physics |
Physics Part-I |
7 |
obtained the amplitude andphaseofcurrentforanLCRseriescircuit using the technique of phasors. But this method of analysing ac circuits suffers from... |
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| Class XII |
Physics |
Physics Part-I |
7 |
current amplitude is given by i = vm = vm m Z 2 2 R + X −CX L) withX c1/ wCandX = L wL.Soif w isvaried,thenataparticularfrequency 2 2 w0, Xc= X L a... |
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