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Question 12 Marks
Discuss $p-n$ junction diode under forward bias.
Answer
→ When an external voltage V is applied across a semi-conductor diode such that $p$-side is connected to the positive terminal of the battery and the $n$-side to the negative terminal (fig. (a)), it is said to be forward biased.
Image
→ Here, the voltage applied to the diode across the two terminals of the depletion region and the direction of the applied voltage
(V) is opposite to the built-in potential (V).
→ As a result, the depletion layer width decreases and the barrier height is reduced (Fig. (b)). The effective barrier height under forward bias is $\left( V _0- V \right)$.
→ If the applied voltage is small, the barrier potential will be reduced only slightly below the equilibrium value and only a small number of carriers in the material - those that happen to be in the uppermost energy levels - will possess enough energy to cross the junction. So the current will be small.
→ If we increase the applied voltage significantly, the height of the barrier potential reduces, and more number of charge carriers gain enough energy to cross the depletion region, due to which the current also increases.
→ "Due to the applied voltage, electrons from the n -side cross the depletion region and reach p -side (Where they are minority carriers). Similarly, holes from the p -side cross the junction and reach the n -side. (Where they are minority carriers.) This process under forward bias is known as minority carrier injection."
→ At the junction boundary, on each side, the minority carrier concentration increases significantly compared to the locations far from the junction.
→ Due to this concentration gradient, the injected electrons on $p$-side diffuse from the junction edge of $p$-side to the other end of $p$ side. Likewise, the injected holes on $n$-side diffuse from the junction edge of $n$-side to the other end of $n$-side. This is shown in fig. below.
Image
→ This motion of charged carriers on either side gives rise to current. The total diode forward current is sum of hole diffusion current and conventional current due to electron diffusion. The magnitude of this current is usually in mA .
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Question 22 Marks
Explain Nuclear binding energy.
Answer
→ The nucleus is made up of neutrons and protons. Therefore, it may be expected that the mass of the nucleus is equal to the total mass of its individual protons and neutrons.
→ But the nuclear mass M is found to be always less than the total mass of its individual protons and neutrons.
→ For example :
$8^{ O ^{16}}$, a nucleus which has 8 neutrons and 8 protons.
Mass of 8 neutrons $=8 \cdot 1.00866 u$
Mass of 8 protons $=8 \cdot 1.00727 u$
Mass of 8 electrons $=8-0.00055 u$
→ Therefore, the expected mass of ${ }_8 O ^{16}$ nucleus
$
\begin{array}{l}
=(8-1.00866+8 \cdot 1.00727) \\
=8(1.00866+1.00727) \\
=8 \cdot 2.01593 u \\
=16.12744 u
\end{array}
$
→ The atomic mass of ${ }_8 O ^{16}$ found from mass spectroscopy experiments is seen to be 15.99493 u .
→ Subtracting the mass of 8 electrons
( $8-0.00055 u=0.0044 u$ ) from this we get the experimental mass of ${ }_8 O ^{16}$ nucleus to be $15.99053 u$.
→ Thus, the mass of the ${ }_8 O ^{16}$ nucleus is less than the total mass of its constituents by
$
(16.12744-15.99053)=0.13691 u
$
→ "The difference in mass of a mucleus and its constituents, $\Delta M$ is called the mass defect" and is given by
$
\Delta M=\left[Z m_p+(A-Z) m_n\right]-M
$
Where, $Z=$ number of protons
$
\begin{array}{l}
A-Z=N=\text { neutron number } \\
m_p \text {-mass of proton } \\
m_n \text {-mass of neutron } \\
M \text { - mass of a nucleus }
\end{array}
$
→ The energy equivalent to this mass defect is called the binding energy of nucleus.
$
\therefore \text { Binding energy } E_b=\Delta M c^2
$
→ Binding energy per nucleon is the binding energy divided by the total number of nucleons.
$
\therefore E_{\text {hn }}=\frac{E_b}{A}
$
→ The binding energy per nucleon gives a measure of the stability of the nucleus.
→ A nucleus for which the value of $E _{b n}$ is comparatively higher is said to be more stable and for a nucleus for which the value of $E _{b n}$ is comparatively less is said to be less stable.
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Question 32 Marks
A hydrogen atom initially in the ground level absorbs a photon, which excites it to the $n=4$ level. Determine the wavelength of photon.
\[\left(h=6.625 \times 10^{-34} Js \& c=3 \times 10^8 ms^{-1}\right)\]
Answer
$ →
n=4
$
$
\begin{array}{l}
\lambda=? \\
v=?
\end{array}
$
→ Total energy of electron
$E _n=-\frac{\frac{13.6}{n^2}}{e}$$e V$....(1)
→ For ground state, $n=1$
$
\begin{array}{l}
E_1=-\frac{13.6}{1^2} eV \\
=-13.6 eV
\end{array}
$
→ Using $n=4$ in equation (1)
$
\begin{array}{l}
E_4=-\frac{-13.6}{(4)^2} eV \\
=\frac{-13.6}{16} e V \\
E_4=-0.85 eV
\end{array}
$
→ Energy of incident photon
$
\begin{array}{l}
E_4-E_1=-0.85-(-13.6) \\
E_4-E_1=12.75 e V
\end{array}
$
But, $E _i- E _f=h v$
$
\begin{array}{l}
h v=12.75 eV \\
\therefore v=\frac{12.75 \times 1.6 \times 10^{-19}}{6.625 \times 10^{-34}} \\
\therefore v=3.08 \times 10^{15} Hz
\end{array}
$
→ Wavelength of incident radiation
$
\begin{array}{l}
\lambda=\frac{c}{v}=\frac{3 \times 10^8}{3.08 \times 10^{15}} \\
\therefore \lambda=0.974 \times 10^{-7} m \\
\therefore \lambda=97.4 nm
\end{array}
$
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Question 42 Marks
Light of frequency $9.21 \times 10^{14} Hz$ is incident on a metal surface. Electrons with a maximum speed $6.0 \times 10^5 ms^{-1}$ are ejected from the surface. What is the threshold frequency for photoemission of electrons?
\[\left(h=6.625 \times 10^{-34} Js\right)\]
Answer

$ →\begin{array}{l}v=9.21 \times 10^{14} Hz \\ v_{\max }=6.0 \times 10^5 m / s \\ → v_0=?\end{array}$
Image
→ According to Einstein's equation,
$\begin{aligned} K _{\max } & =h v-\phi_0 \\ \therefore \frac{1}{2} m v_{\max }^2 & =h v-\phi_0 \quad\left(\because K_{\max }=\frac{1}{2} m v_{\max }^2\right)\end{aligned}$
$\therefore \quad \phi_0=h v-\frac{1}{2} m v_{\max }^2$
$\therefore \quad h v_0=h v-\frac{1}{2} m v_{\max }^2 \quad\left(\because \phi_0=h v_0\right)$
$\therefore \quad v_0=v-\frac{ mV _{\max }^2}{2 h}$
$\therefore \quad v_0=\left(9.21 \times 10^{14}\right)-\left(\frac{9.1 \times 10^{-31} \times\left(6.0 \times 10^5\right)^2}{2 \times 6.625 \times 10^{-34}}\right)$
$\begin{array}{l}v_0=\left(9.21 \times 10^{14}\right)-\left(2.472 \times 10^{14}\right) \\ v_0=6.78 \times 10^{14} Hz\end{array}$
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Question 52 Marks
Derive an expression for the effective focal length of the combination of two thin lenses in contact.
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Question 62 Marks
80 pF capacitor is being charged by an external source. The charging current is constant and equal to 0.15 A . Calculate the rate of change of potential difference between the plates. Also obtain the displacement current across the plates.
Answer
$→
I=C \frac{d V}{d t}
$
where $I =$ Electric Current (A)
$C =$ Capacitance ( F )
$
\begin{array}{l}
\frac{d V}{d t}=\text { Rate of change in electrical condition (Volts Per Second) } \\
C=80 pF=80 \times 10^{-2} F \\
I=0.15 A
\end{array}
$$\frac{d V}{d t}$ is Multiplication of,
$
\begin{array}{l}
0.15=80 \times 10^{-12} \times \frac{d V}{d t} \\
\frac{d V}{d t}=\frac{0.15}{80 \times 10^{-12}}=\frac{0.15}{80 \times 10^{-11}} \\
=1.875 \times 10^9 V / S \\
\text { displacement }=\varepsilon_0 \cdot A \cdot \frac{d E}{d t}
\end{array}
$
displacement (Id displacement) and I is changing in displacement and electrice current
$
I_{\text {displacement }}=I=0.15 A
$
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Question 72 Marks
Derive $\varepsilon= B l \cup$ for motional electromotive force.
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Question 82 Marks
A short bar magnet has a magnetic moment of $0.50 JT ^{-1}$. Calculate the magnitude of the magnetic field produced by the magnet at a distance of 10 cm from the centre of the magnet on
(a) the axis of the magnet and
(b) the equatorial line of the magnet
Answer
$
\begin{aligned}
m= & 0.48 J / T \\
& r=10 cm=0.1 m=10^{-1} m
\end{aligned}
$
(a) Magnetic field on the axis of magnet at distance ' $r$ '
$
\begin{array}{l}
B_1=\frac{\mu_0}{4 \pi} \cdot \frac{2 m}{r^3} \\
B_1=\frac{10^{-7} \times 2 \times 0.48}{10^{-3}} \\
B_1=0.96 \times 10^{-4} T \\
=0.96 G
\end{array}
$
→ Direction of this magnetic field will be in the direction of magnetic moment of the magnet. (Which will be from S to N )
(b) Magnetic field at distance ' $r$ ' on the equatorial line of magnet,
$
\begin{array}{l}
B_2=\frac{\mu_0}{4 \pi} \cdot \frac{m}{r^3} \\
B_2=\frac{10^{-7} \times 0.48}{10^{-3}} \\
B_2=0.48 \times 10^{-4} T \\
=0.48 G
\end{array}
$
→ Direction of this magnetic field will be in the direction opposite to the magnetic moment (Which will be from N to $S$ direction.)
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Question 92 Marks
State the two difficulties in using the galvanometer directly as an ammeter to measure the value of the electric current. What should be done to overcome these difficulties?
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Question 102 Marks
Derive the balance condition for Wheatstone Bridge.
Answer

Image
→ The circuit shown in the figure is called the wheatstone bridge. It uses four resistors $R_1, R_2, R_3$ and $R_4$ out of them three resistors are known and one is unknown, wheatstone bridge is used to find the value of unknown resistance.
→ As shown in the figure, across one pair of diagonally opposite points ( $A$ and $C$ in the figure) a source is connected hence $A C$ is called the battery arm.
→ Between the other two vertices, B and D , a galvanomenter G is connected hence BD is called the galvanometer arm.
→ When battery is connected, the currents flowing through the resistors $R_1, R_2, R_3$ and $R_4$ are $I_1, I_2, I_3$ and $I_4$ respectively.
→ Here, there resistors are chosen in such a way that current flowing through galvanometer is zero ( $I _g=0$ ).
→ When the current flowing through the galvanometer becomes zero, the bridge is said to be in balanced condition.
→ From the figure, in balanced condition
$
I_1=I_3 \text { and } I_2=I_4
$
→ Applying Kirchhoff's loop rule to closed loop A - D - B - A
$
\begin{array}{l}
-I_1 R_1+0+I_2 R_2=0 \\
\therefore I_1 R_1=I_2 R_2 \ldots(1)
\end{array}
$
→ Applying similarly, for closed loop $C - B - D - C$
$
\begin{array}{l}
I_4 R_4+0-I_3 R_3=0 \\
\therefore I_3 R_3=I_4 R_4 \ldots \text { (2) }
\end{array}
$
→ Taking ratio of equation (1) and (2)
$
\therefore \frac{I_1 R_1}{I_3 R_3}=\frac{I_2 R_2}{I_4 R_4}
$
But $I_1=I_3$ and $I_2=I_4$
$
\therefore \frac{R_1}{R_3}=\frac{R_2}{R_4} \text { OR } \frac{R_1}{R_2}=\frac{R_3}{R_4} \ldots(3)
$
→ which is a condition for the whetstone bridge to be in balanced condition.
→ If three resistors $R_1, R_2$ and $R_3$ are known then unknown resistence of $R_4$ is given by
$
R_4=R_3 \cdot \frac{R_2}{R_1} \ldots(4)
$
→ A practical device using this principle is called the meter bridge.
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Question 112 Marks
Derive the relation between electric field and electric potential. Also write two important conclusions concerning this relation.
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Question 122 Marks
Write any four general properties of electric field lines.
Answer
(i) Electric field lines are imaginary curves drawn in such a way that the tangent to it of each point shows the direction of electric field at that point.
(ii) Field lines start from positive charges and end at negative charges. If there is a single charge, they may start or end at infinity.
(iii) In a charge-free region, electric field lines can be taken to be continuous curves without any breaks.
(iv) Two field lines never cross each other.
(v) Electrostatic field lines do not form any closed loops.
(vi) Distribution of electric field lines gives an idea of electric field intensity in that region.
(vii) Field lines of a uniform electric field are mutually parallel and equidistant.
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2 Marks Questions - Physics STD 12 Science Questions - Vidyadip