Showing posts with label Physics Notes. Show all posts
Showing posts with label Physics Notes. Show all posts

12th Physics Volume 1 - Book Back MCQ Test Solutions

PHYSICS VOLUME 1 - BOOK BACK MCQ TEST

Choose the correct Answer

1. The dimension of $1/\mu_{0} \epsilon_{0}$ is........

  • (a) $[LT^{-1}]$
  • (b) $[L^{2}T^{2}]$ ✓ Correct
  • (c) $[L^{-1}T]$
  • (d) $[L^{-2}T^{-2}]$
Solution: The velocity of light $c = \frac{1}{\sqrt{\mu_0 \epsilon_0}}$. Squaring both sides gives $c^2 = \frac{1}{\mu_0 \epsilon_0}$. The dimension of velocity squared is $(LT^{-1})^2 = [L^2 T^{-2}]$.

2. If the amplitude of the magnetic field is $3\times10^{-6}T$, then amplitude of the electric field for a electromagnetic waves is.

  • (a) $100Vm^{-1}$
  • (b) $300Vm^{-1}$
  • (c) $600Vm^{-1}$
  • (d) $900Vm^{-1}$ ✓ Correct
Solution: $E_0 = c \times B_0 = (3 \times 10^8) \times (3 \times 10^{-6}) = 900 V/m$.

3. Which of the following electromagnetic radiations is used for viewing objects through fog.....

  • (a) microwave
  • (b) gamma rays
  • (c) X-rays
  • (d) infrared ✓ Correct
Solution: Infrared radiations are less scattered by atmospheric particles and are used for viewing through fog.

4. Which of the following is false for electromagnetic waves?

  • (a) transverse
  • (b) non-mechanical waves
  • (c) longitudinal ✓ Correct
  • (d) produced by accelerating charges
Solution: Electromagnetic waves are transverse in nature, not longitudinal.

5. Consider an oscillator which has a charged particle oscillating about its mean position with a frequency of 300 MHz. The wavelength of electromagnetic waves produced by this oscillator is...........

  • (a) 1 m ✓ Correct
  • (b) 10 m
  • (c) 100 m
  • (d) 1000 m
Solution: $\lambda = \frac{c}{f} = \frac{3 \times 10^8}{300 \times 10^6} = 1 m$.

6. The following graph shows current versus voltage values of some unknown conductor. What is the resistance of this conductor?

  • (a) 2 Ω ✓ Correct
  • (b) 4 Ω
  • (c) 8 Ω
  • (d) 1 Ω
Solution: Based on the standard V-I graph slope $R = \frac{V}{I}$. From coordinates given in typical plots corresponding to this question: $4/2 = 2 \Omega$.

7. A wire of resistance 2 ohms per meter is bent to form a circle of radius 1m. The equivalent resistance between its two diametrically opposite points, A and B as shown in the figure is........

  • (a) $\pi\Omega$ ✓ Correct
  • (b) $2\pi\Omega$
  • (c) $\pi\Omega$
  • (d) $\pi\Omega$
Solution: Total length $L = 2\pi r = 2\pi(1) = 2\pi$ meters. Total resistance = $2\pi \times 2 = 4\pi \Omega$. The two semicircles are in parallel, each having $2\pi \Omega$. Equivalent resistance $R_{eq} = \frac{2\pi}{2} = \pi \Omega$.

8. A toaster operating at 240 V has a resistance of 120 Ω. Its power is................

  • (a) 400 W
  • (b) 2 W
  • (c) 480 W ✓ Correct
  • (d) 240 W
Solution: $P = \frac{V^2}{R} = \frac{240 \times 240}{120} = 480 W$.

9. A carbon resistor of $(47\pm4.7)k\Omega$ to be marked with rings of different colours for its identification. The colour code sequence will be

  • a) Yellow - Green - Violet - Gold
  • b) Yellow - Violet - Orange - Silver ✓ Correct
  • c) Violet - Yellow - Orange - Silver
  • d) Green - Orange - Violet - Gold
Solution: $47 k\Omega = 47 \times 10^3 \Omega$. 4 = Yellow, 7 = Violet, Multiplier $10^3$ = Orange. Tolerance $\frac{4.7}{47} = 10\%$ = Silver.

10. What is the value of resistance of the following resistor?

  • (a) 100 ΚΩ ✓ Correct
  • (b) 10 ΚΩ
  • (c) 1 ΚΩ
  • (d) 1000 ΚΩ
Solution: Referencing typical textbook diagrams for this specific question, the standard answer corresponding to the missing image is 100 kΩ.

11. The magnetic field at the centre O of the following current loop is

  • (a) $\mu_0 I/4r$ INWARDS ✓ Correct
  • (b) $\mu_0 I/4r$ OUTWARDS
  • (c) $\mu_0 I/2r$ INWARDS
  • (d) $\mu_0 I/2r$ OUTWARDS
Solution: For a semi-circular current loop, $B = \frac{\mu_0 I}{4r}$. Applying the right-hand rule, the field is directed inwards.

12. An electron moves in a straight line inside a charged parallel plate capacitor of uniform charge density $\sigma$. The time taken by the electron to cross the parallel plate capacitor undeflected when the plates of the capacitor are kept under constant magnetic field of induction B is

  • (a) $\frac{\epsilon_0 elB}{\sigma}$
  • (b) $\frac{\epsilon_0 lB}{\sigma}$ ✓ Correct
  • (c) $\frac{\epsilon_0 IB}{e\sigma}$
  • (d) $\frac{\epsilon_0 IB}{\sigma}$
Solution: Undeflected velocity $v = \frac{E}{B}$. Electric field $E = \frac{\sigma}{\epsilon_0}$. Hence $v = \frac{\sigma}{\epsilon_0 B}$. Time taken $t = \frac{l}{v} = \frac{l \epsilon_0 B}{\sigma}$.

13. A particle having mass m and charge q accelerated through a potential difference V. Find the force experienced when it is kept under perpendicular magnetic field B.............

  • (a) $\sqrt{\frac{2q^{3}BV}{m}}$
  • (b) $\sqrt{\frac{q^{3}B^{2}V}{2m}}$
  • (c) $\sqrt{\frac{2q^{3}B^{2}V}{m}}$ ✓ Correct
  • (d) $\sqrt{\frac{2q^{3}BV}{m^{3}}}$
Solution: Kinetic energy $K = qV \implies \frac{1}{2}mv^2 = qV \implies v = \sqrt{\frac{2qV}{m}}$. Magnetic force $F = qvB = qB \sqrt{\frac{2qV}{m}} = \sqrt{\frac{2q^3 B^2 V}{m}}$.

14. A circular coil of radius 5 cm and 50 turns carries a current of 3 ampere. The magnetic dipole moment of the coil is nearly..............

  • (a) $1.0~amp-m^{2}$
  • (b) $1.2~amp-m^{2}$ ✓ Correct
  • (c) $0.5~amp-m^{2}$
  • (d) $0.8~amp-m^2$
Solution: Magnetic moment $M = N I A = 50 \times 3 \times (\pi \times 0.05^2) \approx 1.1775 \approx 1.2 Am^2$.

15. A thin insulated wire forms a plane spiral of $N=100$ tight turns carrying a current $I=8$ m A (milli ampere). The radii of inside and outside turns are $a=50~mm$ and $b=100$ mm respectively. The magnetic induction at the centre of the spiral is

  • (a) $5~\mu T$
  • (b) $7~\mu T$ ✓ Correct
  • (c) $8~\mu T$
  • (d) $10~\mu T$
Solution: Magnetic field at the center of a spiral coil: $B = \frac{\mu_0 N I}{2(b-a)} \ln\left(\frac{b}{a}\right)$. Substituting values yields approximately $7 \mu T$.

16. Two identical point charges of magnitude -q are fixed as shown in the figure below. A third charge +q is placed midway between the two charges at the point P. Suppose this charge +q is displaced a small distance from the point P in the directions indicated by the arrows, in which direction(s) will +q be stable with respect to the displacement?

  • (a) A1 and A2 ✓ Correct
  • (b) B1 and B2
  • (c) both direction
  • (d) No stable
Solution: A positive charge placed midway between two identical negative charges is in stable equilibrium for displacements perpendicular to the axis joining them (A1 and A2).

17. Which charge configuration produces a uniform electric field?

  • (a) point charge
  • (b) uniformly charged infinite line
  • (c) uniformly charged infinite plane ✓ Correct
  • (d) uniformly charged spherical shell
Solution: A uniformly charged infinite plane sheet produces a constant uniform electric field $E = \frac{\sigma}{2\epsilon_0}$.

18. What is the ratio of the charges q1/ q2 for the following electric field line pattern?

  • (a) $1/5$
  • (b) $25/11$
  • (c) 5
  • (d) $11/25$ ✓ Correct
Solution: The magnitude of charge is proportional to the number of electric field lines originating or terminating on it. Based on the standard textbook figure for this problem, the ratio of lines is 11/25.

19. An electric dipole is placed at an alignment angle of $30^{\circ}$ with an electric field of $2\times10^{5}NC^{-1}.$ It experiences a torque equal to 8 Nm. The charge on the dipole if the dipole length is 1 cm is.

  • (a) 4 mC
  • (b) 8 mC ✓ Correct
  • (c) 5 mC
  • (d) 7 mC
Solution: Torque $\tau = pE \sin\theta = (q \times 2a)E \sin\theta$. Substituting: $8 = q \times 10^{-2} \times 2 \times 10^5 \times \sin(30^{\circ}) \implies q = 8 \times 10^{-3} C = 8 mC$.

20. Four Gaussian surfaces are given below with charges inside each Gaussian surface. Rank the electric flux through each Gaussian surface in increasing order.

  • (a) $D
  • (b) $A
  • (c) $C
  • (d) $D>C>B>A$
Solution: According to Gauss's Law, flux $\Phi = \frac{q_{enclosed}}{\epsilon_0}$. The ranking strictly depends on the net charge enclosed inside the given standard visual volumes (A < B=C < D).

21. An electron moves on a straight line path XY as shown in the figure. The coil abcd is adjacent to the path of the electron. What will be the direction of current, if any, induced in the coil?

  • (a) The current will reverse its direction as the electron goes past the coil ✓ Correct
  • (b) No current will be induced
  • (c) abcd
  • (d) adcb
Solution: As the electron approaches the coil, the magnetic flux into the page increases. According to Lenz's law, the induced current will oppose this change, flowing counterclockwise (abcd). As the electron moves away, the flux decreases, and the induced current reverses direction to clockwise (adcb) to oppose the decrease.

22. A thin semi-circular conducting ring (PQR) of radius r is falling with its plane vertical in a horizontal magnetic field B, as shown in the figure. The potential difference developed across the ring when its speed v, is......

  • (a) zero
  • (b) $Bv\pi r^{2} / 2$ and P is at higher potential
  • (c) $\pi rBv$ and R is at higher potential
  • (d) $2rBv$ and R is at higher potential ✓ Correct
Solution: The motional emf developed is given by $e = B \cdot l_{eff} \cdot v$. The effective length $l_{eff}$ of the semi-circular ring is its diameter, $2r$. Thus, $e = B(2r)v = 2rBv$. Using Fleming's Right Hand Rule (or the Lorentz force on positive charges $q(\vec{v} \times \vec{B})$), the end R is at a higher potential.

23. The flux linked with a coil at any instant t is given by $\phi_{B}=10t^{2}-50t+250$. The induced emf at $t=3$ s is................

  • (a) -190 V
  • (b) -10 V ✓ Correct
  • (c) 10 V
  • (d) 190 V
Solution: By Faraday's law of induction, $e = -\frac{d\phi_{B}}{dt}$.
$e = -\frac{d}{dt}(10t^{2} - 50t + 250) = -(20t - 50)$.
At $t = 3$ s, $e = -(20(3) - 50) = -(60 - 50) = -10$ V.

24. When the current changes from +2A to -2A in 0.05 s, an emf of 8 V is induced in a coil. The co-efficient of self-induction of the coil is........

  • (a) 0.2 H
  • (b) 0.4 H
  • (c) 0.8 H
  • (d) 0.1 H ✓ Correct
Solution: Change in current $di = -2 - 2 = -4$ A. Time interval $dt = 0.05$ s. Induced emf $e = 8$ V.
Using the formula $e = -L\frac{di}{dt}$, we get $8 = -L\left(\frac{-4}{0.05}\right)$.
$8 = L(80) \implies L = \frac{8}{80} = 0.1$ H.

25. The current i flowing in a coil varies with time as shown in the figure. The variation of induced emf with time would be...............

  • (a) Graph with constant negative, then zero, then constant positive emf ✓ Correct
  • (b) Graph variation
  • (c) Graph variation
  • (d) Graph variation
Solution: Induced emf $e = -L\frac{di}{dt}$. During the first interval, current increases linearly, so $\frac{di}{dt}$ is a positive constant, making $e$ a negative constant. In the middle interval, current is constant ($\frac{di}{dt} = 0$), so $e = 0$. In the last interval, current decreases linearly ($\frac{di}{dt}$ is negative), making $e$ a positive constant. This corresponds to graph (a).

26. The total electric flux for the following closed surface which is kept inside water.....

  • (a) $\frac{80q}{\epsilon_{0}}$
  • (b) $\frac{q}{40\epsilon_{0}}$ ✓ Correct
  • (c) $\frac{q}{80\epsilon_{0}}$
  • (d) $\frac{q}{160\epsilon_{0}}$
Solution: The net charge enclosed is $q_{net} = +2q + q - q = +2q$.
By Gauss's Law, $\Phi = \frac{q_{net}}{\epsilon} = \frac{2q}{\epsilon_{r}\epsilon_{0}}$. For water, the relative permittivity $\epsilon_{r} \approx 80$.
Therefore, $\Phi = \frac{2q}{80\epsilon_{0}} = \frac{q}{40\epsilon_{0}}$.

27. Two identical conducting balls having positive charges q1 and q2 are separated by a centre to centre distance r. If they are made to touch each other and then separated to the same distance, the force between them will be

  • (a) less than before
  • (b) same as before
  • (c) more than before ✓ Correct
  • (d) zero
Solution: Initially, force $F \propto q_{1}q_{2}$. After touching, the charges redistribute equally to $q' = \frac{q_{1}+q_{2}}{2}$. The new force $F' \propto \left(\frac{q_{1}+q_{2}}{2}\right)^{2}$. Since the square of the arithmetic mean is always strictly greater than the geometric mean for unequal positive numbers, $F' > F$.

28. Rank the electrostatic potential energies for the given system of charges in increasing order.

  • (a) $1=4<2<3$ ✓ Correct
  • (b) $2=4<3<1$
  • (c) $2=3<1<4$
  • (d) $3<1<2<4$
Solution: Evaluating standard potential energy configurations $U = \frac{1}{4\pi\epsilon_{0}} \frac{q_1 q_2}{r}$, potential energy depends directly on the product of charges and inversely on the distance. Matching standard textbook sequences yields the rank order $1=4 < 2 < 3$.

29. An electric field $E=10\times\hat{i}$ exists in a certain region of space. Then the potential difference $V=V_{0}-V_{A}$ where $V_{0}$ is the potential at the origin and $V_{A}$ is the potential at $x=2$ m is...........

  • (a) 10 V
  • (b) -20 V
  • (c) 20 V ✓ Correct
  • (d) -10 V
Solution: Potential difference is given by $\Delta V = -\int \vec{E} \cdot d\vec{x}$.
$V_{A} - V_{0} = - \int_{0}^{2} 10 \, dx = -10[x]_{0}^{2} = -20$ V.
Therefore, $V_{0} - V_{A} = 20$ V.

30. A thin conducting spherical shell of radius R has a charge Q which is uniformly distributed on its surface. The correct plot for electrostatic potential due to this spherical shell is..........

  • (a) Graph A
  • (b) Graph B (Constant inside, 1/r outside) ✓ Correct
  • (c) Graph C
  • (d) Graph D
Solution: Inside a conducting spherical shell ($r < R$), the electric field is zero, so the potential remains constant and equal to the value at the surface ($V = \frac{1}{4\pi\epsilon_{0}}\frac{Q}{R}$). Outside the shell ($r > R$), the potential varies inversely with distance ($V \propto \frac{1}{r}$). This matches graph (b).

31. The electric and the magnetic fields, associated with an electromagnetic wave, propagating along negative X axis can be represented by

  • (a) $\vec{E}=E_{0}\hat{j}$ and $\vec{B}=B_{0}\hat{k}$
  • (b) $\vec{E}=E_{0}\hat{k}$ and $\vec{B}=B_{0}\hat{j}$ ✓ Correct
  • (c) $\vec{E}=E_{0}\hat{i}$ and $\vec{B}=B_{0}\hat{j}$
  • (d) $\vec{E}=E_{0}\hat{j}$ and $\vec{B}=B_{0}\hat{i}$
Solution: The direction of propagation is given by the Poynting vector, which is parallel to $\vec{E} \times \vec{B}$. For propagation along the negative X axis ($-\hat{i}$), we need the cross product to yield $-\hat{i}$. Testing option (b): $\hat{k} \times \hat{j} = -\hat{i}$, which satisfies the condition.

32. In an electromagnetic wave travelling in free space the rms value of the electric field is $3 V m^{-1}$. The peak value of the magnetic field is.

  • (a) $1.414\times10^{-8}T$ ✓ Correct
  • (b) $1.0\times10^{-8}T$
  • (c) $2.828\times10^{-8}T$
  • (d) $2.0\times10^{-8}T$
Solution: The peak electric field $E_{0} = \sqrt{2} E_{rms} = 3\sqrt{2}$ V/m. The peak magnetic field $B_{0} = \frac{E_{0}}{c} = \frac{3\sqrt{2}}{3\times10^{8}} = \sqrt{2}\times10^{-8}$ T. Since $\sqrt{2} \approx 1.414$, $B_{0} = 1.414 \times 10^{-8}$ T.

33. An e.m. wave is propagating in a medium with a velocity v. The instantaneous oscillating electric field of this e.m. wave is along +y-axis, then the direction of oscillating magnetic field of the e.m. wave will be along:

  • (a) -y direction
  • (b) -x direction
  • (c) +z direction ✓ Correct
  • (d) -z direction
Solution: Assuming standard Cartesian wave propagation along the +x axis (velocity $\vec{v}$), the direction of wave travel is given by $\vec{E} \times \vec{B}$. With $\vec{E}$ along $+\hat{j}$ (y-axis), $\hat{j} \times \vec{B}_{dir} = \hat{i}$. This is satisfied when $\vec{B}_{dir} = \hat{k}$ (+z direction).

34. If the magnetic monopole exists, then which of the Maxwell's equation to be modified?.

  • (a) $\oint\vec{E}\cdot d\vec{A}=\frac{Q_{encl}}{\epsilon_{0}}$
  • (b) $\oint\vec{B}\cdot d\vec{A}=0$ ✓ Correct
  • (c) $\oint\vec{B}\cdot d\vec{l}=\mu_{0}I_{encl}+\mu_{0}\epsilon_{0}\frac{d}{dt}\oint\vec{E}\cdot d\vec{A}$
  • (d) $\oint\vec{E}\cdot d\vec{l}=-\frac{d}{dt}\phi_{B}$
Solution: Gauss's Law for magnetism, $\oint\vec{B}\cdot d\vec{A}=0$, states that magnetic monopoles do not exist. If they were to exist, this equation would need to be modified to $\oint\vec{B}\cdot d\vec{A} = \mu_{0} q_{m}$, where $q_{m}$ is the magnetic monopole charge.

35. Fraunhofer lines are an example of

  • (a) line emission spectrum
  • (b) line absorption spectrum ✓ Correct
  • (c) band emission spectrum
  • (d) band absorption spectrum
Solution: Fraunhofer lines are dark absorption lines seen in the continuous spectrum of the sun, caused by cooler gases in the solar atmosphere absorbing specific wavelengths. Therefore, they are an example of a line absorption spectrum.

36. Two wires of A and B with circular cross section are made up of the same material with equal lengths. Suppose $R_{A}=3 R_{B}$, then what is the ratio of radius of wire A to that of B?

  • (a) 3
  • (b) $\sqrt{3}$
  • (c) $1/\sqrt{3}$ ✓ Correct
  • (d) $1/3$
Solution: Resistance $R = \rho \frac{l}{A} = \rho \frac{l}{\pi r^{2}}$. Since the wires are of the same material and length, $R \propto \frac{1}{r^{2}}$.
$\frac{R_{A}}{R_{B}} = \left(\frac{r_{B}}{r_{A}}\right)^{2}$. Given $R_{A} = 3 R_{B}$, so $\frac{R_{A}}{R_{B}} = 3$.
$3 = \left(\frac{r_{B}}{r_{A}}\right)^{2} \implies \frac{r_{A}}{r_{B}} = \frac{1}{\sqrt{3}}$.

37. A wire connected to a power supply of 230 V has power dissipation P1. Suppose the wire is cut into two equal pieces and connected parallel to the same power supply. In this case power dissipation is P2. The ratio $P_{1}/P_{2}$ is

  • (a) 1
  • (b) 2
  • (c) 3
  • (d) 1/4 ✓ Correct
Solution: Initial power $P_{1} = \frac{V^{2}}{R}$. Cutting the wire in half yields two resistors of resistance $R/2$. Connecting them in parallel gives an equivalent resistance $R_{eq} = \frac{(R/2)}{2} = \frac{R}{4}$. New power $P_{2} = \frac{V^{2}}{R_{eq}} = \frac{V^{2}}{R/4} = 4\frac{V^{2}}{R} = 4 P_{1}$. The ratio $P_{1}/P_{2} = 1/4$.

38. In India electricity is supplied for domestic use at 220 V. It is supplied at 110 V in USA. If the resistance of a 60W bulb for use in India is R, the resistance of a 60W bulb for use in USA will be.....

  • (a) R
  • (b) 2R
  • (c) R/4 ✓ Correct
  • (d) R/2
Solution: From $P = \frac{V^{2}}{R}$, we have $R = \frac{V^{2}}{P}$.
For India: $R = \frac{220^{2}}{60}$. For USA: $R_{USA} = \frac{110^{2}}{60}$.
Ratio $\frac{R_{USA}}{R} = \left(\frac{110}{220}\right)^{2} = \left(\frac{1}{2}\right)^{2} = \frac{1}{4}$. Thus, $R_{USA} = \frac{R}{4}$.

39. In a large building, there are 15 bulbs of 40 W, 5 bulbs of 100 W, 5 fans of 80 W and 1 heater of 1k W are connected. The voltage of electric mains is 220 V. The maximum capacity of the main fuse of the building will be.

  • (a) 14 A
  • (b) 8 A
  • (c) 10 A
  • (d) 12 A ✓ Correct
Solution: Total power $P = (15 \times 40) + (5 \times 100) + (5 \times 80) + 1000 = 600 + 500 + 400 + 1000 = 2500$ W.
Total current drawn $I = \frac{P}{V} = \frac{2500}{220} \approx 11.36$ A. The safe fuse capacity just above this value is 12 A.

40. There is a current of 1.0 A in the circuit shown below. What is the resistance of P?

  • (a) 1.5 Ω
  • (b) 2.5 Ω
  • (c) 3.5 Ω ✓ Correct
  • (d) 4.5 Ω
Solution: Let the total resistance of the circuit be $R_{eq}$. By Ohm's law, $R_{eq} = \frac{V}{I} = \frac{9}{1.0} = 9 \, \Omega$. Based on a standard series loop interpretation of the circuit ($3 \, \Omega + 2.5 \, \Omega + P$), we have $3 + 2.5 + P = 9$. Thus, $P = 9 - 5.5 = 3.5 \, \Omega$.

Key Concepts of Nuclear Physics: Important Points to Remember for Class 10 Science

Points to Remember - Nuclear Physics | Science

Nuclear Physics (Science)

Points to Remember

  • This phenomenon of spontaneous emission of radiation from certain elements on its own is called 'natural radioactivity'.
  • Curie is defined as the quantity of a radioactive substance, which undergoes 3.7 × 1010 disintegrations in one second. This is actually close to the activity of 1 g of radium-226.
  • Rutherford (Rd) is defined as the quantity of a radioactive substance which produces 106 disintegrations in one second. 1 Rd = 106 disintegrations per second.
  • The SI unit of radioactivity is becquerel. It is defined as the quantity of one disintegration per second.
  • Helium nucleus (2He4) consisting of two protons and two neutrons is known as alpha particle.
  • Beta particles are electrons (-1e0), which are the basic elementary particles present in all atoms.
  • Gamma rays are electromagnetic waves consisting of photons.
  • A nuclear reaction in which an unstable parent nucleus emits an alpha particle and forms a stable daughter nucleus is called as 'alpha decay'.
  • A nuclear reaction in which an unstable parent nucleus emits a beta particle and forms a stable daughter nucleus is called as 'beta decay'.
  • The process of breaking (splitting) up of a heavier nucleus into two smaller nuclei with the release of a large amount of energy is called 'nuclear fission'.
  • The energy released in a nuclear fission process is about 200 MeV.
  • There are some radioactive elements which can be converted into a fissionable material. They are called as 'fertile materials'. e.g. Uranium-238, Thorium-232, Plutonium-240.
  • Controlled chain reaction is used in a nuclear reactor to produce energy in a sustained and controlled manner.
  • The process in which two lighter nuclei combine to form a heavier nucleus is termed as 'nuclear fusion'.
  • Nuclear fusion or thermonuclear reaction is the source of light and heat energy in the Sun and other stars.
  • The safe limit of receiving the radiation is about 100 mR per week.

Nuclear Fission and Fusion: Definitions, Chain Reactions, Critical Mass, and Atom Bombs

Nuclear Fission & Fusion

NUCLEAR FISSION

1. Definition

In 1939, German Scientist Otto Hahn and F.Strassman discovered that when a uranium nucleus is bombarded with a neutron, it breaks up into two smaller nuclei of comparable mass along with the emission of a few neutrons and energy. This process of breaking (splitting) up of a heavier nucleus into two smaller nuclei with the release of a large amount of energy and a few neutrons is called 'nuclear fission'.

E.g.: Nuclear fission of a uranium nucleus (U235)

$$ ^{235}_{92}U + ^{1}_{0}n \rightarrow ^{141}_{56}Ba + ^{92}_{36}Kr + 3^{1}_{0}n + Q (\text{energy}) $$

The average energy released in each fission process is about 3.2 × 10-11 J. Nuclear fission is pictorially represented in Figure 6.2.

Figure 6.2 Nuclear fission diagram

2. Fissionable materials

A fissionable material is a radioactive element, which undergoes fission in a sustained manner when it absorbs a neutron. It is also termed as 'fissile material'.

E.g.: U235, plutonium (Pu239 and Pu241)

All isotopes of uranium do not undergo nuclear fission when they absorb a neutron. For example, natural uranium consists of 99.28 % of 92U238 and 0.72 % of 92U235. Of these two, U238 does not undergo fission whereas U235 undergoes fission. Hence, U235 is a fissionable material and U238 is non-fissionable.

There are some radioactive elements, which can be converted into fissionable material. They are called as fertile materials.

E.g.: Uranium-238, Thorium-232, Plutonium-240.

3. Chain Reaction

A uranium nucleus (U-235) when bombarded with a neutron undergoes fission producing three neutrons. These three neutrons in turn can cause fission in three other uranium nuclei present in the sample, thus producing nine neutrons. These nine neutrons in turn may produce twenty seven neutrons and so on. This is known as 'chain reaction'. A chain reaction is a self-propagating process in which the number of neutrons goes on multiplying rapidly almost in a geometrical progression.

Two kinds of chain reactions are possible. They are: (i) controlled chain reaction and (ii) uncontrolled chain reaction.

(a) Controlled chain reaction

In the controlled chain reaction the number of neutrons released is maintained to be one. This is achieved by absorbing the extra neutrons with a neutron absorber leaving only one neutron to produce further fission. Thus, the reaction is sustained in a controlled manner. The energy released due to a controlled chain reaction can be utilized for constructive purposes. Controlled chain reaction is used in a nuclear reactor to produce energy in a sustained and controlled manner.

(b) Uncontrolled chain reaction

In the uncontrolled chain reaction the number of neutrons multiplies indefinitely and causes fission in a large amount of the fissile material. This results in the release of a huge amount of energy within a fraction of a second. This kind of chain reaction is used in the atom bomb to produce an explosion. Figure 6.3 represents an uncontrolled chain reaction.

Figure 6.3 Uncontrolled chain reaction diagram

4. Critical Mass

During a nuclear fission process, about 2 to 3 neutrons are released. But, all these neutrons may not be available to produce further fission. Some of them may escape from the system, which is termed as 'leakage of neutrons' and some may be absorbed by the non-fissionable materials present in the system. These two factors lead to the loss of neutrons. To sustain the chain reaction, the rate of production of neutrons due to nuclear fission must be more than the rate of its loss. This can be achieved only when the size (i.e., mass) of the fissionable material is equal to a certain optimum value. This is known as 'critical mass'.

The minimum mass of a fissile material necessary to sustain the chain reaction is called 'critical mass (mc)'. It depends on the nature, density and the size of the fissile material.

If the mass of the fissile material is less than the critical mass, it is termed as 'subcritical'. If the mass of the fissile material is more than the critical mass, it is termed as 'supercritical'.

5. Atom bomb

The atom bomb is based on the principle of uncontrolled chain reaction. In an uncontrolled chain reaction, the number of neutrons and the number of fission reactions multiply almost in a geometrical progression. This releases a huge amount of energy in a very small time interval and leads to an explosion.

Structure:

An atom bomb consists of a piece of fissile material whose mass is subcritical. This piece has a cylindrical void. It has a cylindrical fissile material which can fit into this void and its mass is also subcritical. When the bomb has to be exploded, this cylinder is injected into the void using a conventional explosive. Now, the two pieces of fissile material join to form the supercritical mass, which leads to an explosion. The structure of an atom bomb is shown in Figure 6.4

Figure 6.4 Atom bomb structure

During this explosion tremendous amount of energy in the form of heat, light and radiation is released. A region of very high temperature and pressure is formed in a fraction of a second along with the emission of hazardous radiation like γ rays, which adversely affect the living creatures. This type of atom bombs were exploded in 1945 at Hiroshima and Nagasaki in Japan during the World War II.

NUCLEAR FUSION

You have learnt that energy can be produced when a heavy nucleus is split up into two smaller nuclei. Similarly, energy can be produced when two lighter nuclei combine to form a heavier nucleus. This phenomenon is known as nuclear fusion.

1. Definition

The process in which two lighter nuclei combine to form a heavier nucleus is termed as 'nuclear fusion'.

E.g.:

$$ ^{2}_{1}H + ^{2}_{1}H \rightarrow ^{4}_{2}He + Q (\text{Energy}) $$

Here, 1H2 represents an isotope of hydrogen known as 'deuterium'. The average energy released in each fusion reaction is about 3.84 × 10-12 J. Figure 6.5 represents this.

Figure 6.5 Nuclear fusion diagram

The mass of the daughter nucleus formed during a nuclear reaction (fission and fusion) is lesser than the sum of the masses of the two parent nuclei. This difference in mass is called mass defect. This mass is converted into energy, according to the mass-energy equivalence. This concept of mass-energy equivalence was proposed by Einstein in 1905. It stated that mass can be converted into energy and vice versa. The relation between mass and energy proposed by Einstein is E = mc2 where c is the velocity of light in vacuum and is equal to 3 × 108 ms–1.

2. Conditions necessary for nuclear fusion

Earth’s atmosphere contains a small trace of hydrogen. If nuclear fusion is a spontaneous process at normal temperature and pressure, then a number of fusion processes would happen in the atmosphere which may lead to explosions. But, we do not encounter any such explosions. Can you explain why?

The answer is that nuclear fusion can take place only under certain conditions.

Nuclear fusion is possible only at an extremely high temperature of the order of 107 to 109 K and a high pressure to push the hydrogen nuclei closer to fuse with each other. Hence, it is named as 'Thermonuclear reaction'.

3. Stellar Energy

The stars like our Sun emit a large amount of energy in the form of light and heat. This energy is termed as the stellar energy. Where does this high energy come from? All stars contain a large amount of hydrogen. The surface temperature of the stars is very high which is sufficient to induce fusion of the hydrogen nuclei.

Fusion reaction that takes place in the cores of the Sun and other stars results in an enormous amount of energy, which is called as 'stellar energy. Thus, nuclear fusion or thermonuclear reaction is the source of light and heat energy in the Sun and other stars.

4. Hydrogen Bomb

Hydrogen bomb is based on the principle of nuclear fusion. A hydrogen bomb is always designed to have an inbuilt atom bomb which creates the high temperature and pressure required for fusion when it explodes. Then, fusion takes place in the hydrogen core and leads to the release of a very large amount of energy in an uncontrolled manner. The energy released in a hydrogen bomb (or fusion bomb) is much higher than that released in an atom bomb (or fission bomb).

Features of Nuclear Fission and Nuclear Fusion

NUCLEAR FISSION

  • The process of breaking up (splitting) of a heavy nucleus into two smaller nuclei is called 'nuclear fission'.
  • Can be performed at room temperature.
  • Alpha, beta and gamma radiations are emitted.
  • Fission leads to emission of gamma radiation. This triggers the mutation in the human gene and causes genetic transform diseases.

NUCLEAR FUSION

  • Nuclear fusion is the combination of two lighter nuclei to form a heavier nucleus.
  • Extremely high temperature and pressure is needed.
  • Alpha rays, positrons, and neutrinos are emitted.
  • Only light and heat energy is emitted.
Table 6.3 Features of Nuclear fission and nuclear fusion

Doppler Effect in Sound: Conditions, Applications & Solved Problems

Doppler Effect - Conditions, Applications, Solved Example Problems

DOPPLER EFFECT

The whistle of a fast moving train appears to increase in pitch as it approaches a stationary listener and it appears to decrease as the train moves away from the listener. This apparent change in frequency was first observed and explained by Christian Doppler (1803-1853), an Austrian Mathematician and Physicist. He observed that the frequency of the sound as received by a listener is different from the original frequency produced by the source whenever there is a relative motion between the source and the listener. This is known as Doppler effect. This relative motion could be due to various possibilities as follows:

  1. The listener moves towards or away from a stationary source
  2. The source moves towards or away from a stationary listener
  3. Both source and listener move towards or away from one other
  4. The medium moves when both source and listener are at rest

For simplicity of calculation, it is assumed that the medium is at rest. That is the velocity of the medium is zero.

Let S and L be the source and the listener moving with velocities $v_S$ and $v_L$ respectively. Consider the case of source and listener moving towards each other (Figure 5.7). As the distance between them decreases, the apparent frequency will be more than the actual source frequency.

Figure 5.7 Source and listener moving towards each other

Let n and n' be the frequency of the sound produced by the source and the sound observed by the listener respectively. Then, the expression for the apparent frequency n' is:

Doppler Effect Formula: n' = [ (v + vL) / (v - vS) ] n

Here, v is the velocity of sound waves in the given medium. Let us consider different possibilities of motions of the source and the listener. In all such cases, the expression for the apparent frequency is given in table 5.2.

Table 5.2: Expression for Apparent Frequency

Table 5.2 Part 1: Expression for apparent frequency due to Doppler effect Table 5.2 Part 2: Expression for apparent frequency due to Doppler effect

Suppose the medium (say wind) is moving with a velocity W in the direction of the propagation of sound. For this case, the velocity of sound, ‘v’ should be replaced with (v + W). If the medium moves in a direction opposite to the propagation of sound, then ‘v’ should be replaced with (v – W).

Solved problems

1. A source producing a sound of frequency 90 Hz is approaching a stationary listener with a speed equal to (1/10) of the speed of sound. What will be the frequency heard by the listener?

Solution:

When the source is moving towards the stationary listener, the expression for apparent frequency is:

Solution to problem 1 on Doppler effect

2. A source producing a sound of frequency 500 Hz is moving towards a listener with a velocity of 30 m s–1. The speed of the sound is 330 m s–1. What will be the frequency heard by listener?

Solution:

When the source is moving towards the stationary listener, the expression for apparent frequency is:

Solution to problem 2 on Doppler effect

3. A source of sound is moving with a velocity of 50 m s–1 towards a stationary listener. The listener measures the frequency of the source as 1000 Hz. What will be the apparent frequency of the source when it is moving away from the listener after crossing him? (velocity of sound in the medium is 330 m s–1)

Solution:

When the source is moving towards the stationary listener, the expression for apparent frequency is:

Solution step 1 for problem 3 on Doppler effect

n = 848.48 Hz.

The actual frequency of the sound is 848.48 Hz. When the source is moving away from the stationary listener, the expression for apparent frequency is:

Solution step 2 for problem 3 on Doppler effect

= 736.84 Hz

4. A source and listener are both moving towards each other with a speed v/10 where v is the speed of sound. If the frequency of the note emitted by the source is f, what will be the frequency heard by the listener?

Solution:

When source and listener are both moving towards each other, the apparent frequency is:

Solution to problem 4 on Doppler effect

5. At what speed should a source of sound move away from a stationary observer so that observer finds the apparent frequency equal to half of the original frequency?

Solution:

When the source is moving away from the stationary listener, the expression for the apparent frequency is:

Solution to problem 5 on Doppler effect

Conditions for no Doppler effect

Under the following circumstances, there will be no Doppler effect and the apparent frequency as heard by the listener will be the same as the source frequency.

  • When source (S) and listener (L) both are at rest.
  • When S and L move in such a way that distance between them remains constant.
  • When source S and L are moving in mutually perpendicular directions.
  • If the source is situated at the center of the circle along which the listener is moving.

Applications of Doppler effect

(a) To measure the speed of an automobile

An electromagnetic wave is emitted by a source attached to a police car. The wave is reflected by a moving vehicle, which acts as a moving source. There is a shift in the frequency of the reflected wave. From the frequency shift, the speed of the car can be determined. This helps to track the over speeding vehicles.

(b) Tracking a satellite

The frequency of radio waves emitted by a satellite decreases as the satellite passes away from the Earth. By measuring the change in the frequency of the radio waves, the location of the satellites is studied.

(c) RADAR (RAdio Detection And Ranging)

In RADAR, radio waves are sent, and the reflected waves are detected by the receiver of the RADAR station. From the frequency change, the speed and location of the aeroplanes and aircrafts are tracked.

(d) SONAR

In SONAR, by measuring the change in the frequency between the sent signal and received signal, the speed of marine animals and submarines can be determined.

Important Points to Remember for Electricity | Science Class 10

Points to Remember - Electricity | Science

Electricity (Science) - Points to Remember

  • The magnitude of current is defined as the rate of flow of charges in a conductor.
  • The SI unit of electric current is ampere (A).
  • The SI unit of electric potential and potential difference is volt (V).
  • An electric circuit is a network of electrical components, which forms a continuous and closed path for an electric current to pass through it.
  • The parameters of conductors like its length, area of cross-section and material, affect the resistance of the conductor.
  • SI unit of electrical resistivity is ohm metre. The resistivity is a constant for a given material.
  • The reciprocal of electrical resistivity of a material is called its electrical conductivity. \(\sigma = 1/\rho\)
  • The passage of electric current through a wire results in the production of heat.
  • This phenomenon is called heating effect of current.
  • One horse power is equal to 746 watts.
  • The function of a fuse wire or a MCB is to protect the house hold electrical appliances from excess current due to overloading or a short circuit.

Electricity - An Introduction | Class 10 Science Chapter 4

Electricity - Introduction

INTRODUCTION

You have already learnt about electricity in your lower classes, haven’t you? Well, electricity deals with the flow of electric charges through a conductor. As a common term it refers to a form of energy. The usage of electric current in our day to day life is very important and indispensable. You are already aware of the fact that it is used in houses, educational institutions, hospitals, industries, etc. Therefore, its generation and transmission becomes a very crucial aspect of our life. In this lesson you will learn various terms used in understanding the concept of electricity. Eventually, you will realise the importance of the applications of electricity in day to day situations.

A concept map outlining the key topics in the chapter of Electricity
Concept Map for Electricity Chapter

Related Topics & Keywords:

Introduction 10th Science Chapter 4 Electricity Study Material Lecturing Notes Assignment Reference Explanation

Points to Remember: Thermal Physics - Key Concepts & Definitions for Science Students

Thermal Physics

Key Points to Remember

Fundamental Concepts

  1. The SI unit of heat energy absorbed or evolved is joule (J)
  2. Heat always flows from a system at higher temperature to a system at lower temperature.
  3. Temperature is defined as the degree of hotness of a body. The SI unit of temperature is kelvin (K).
  4. All the substances will undergo one or more of the following changes when heated:
    1. Temperature of the substance rises.
    2. The substance may change state from solid to liquid or gas.
    3. The substance will expand when heated.
  5. All forms of matter (solid, liquid and gas) undergo expansion on heating.
  6. For a given rise in temperature, a liquid will have more expansion than a solid and a gaseous substance has the highest expansion than the other two.
  7. If a liquid is heated directly without using any container, then the expansion that you observe is termed as real expansion of the liquid.
  8. The expansion of a liquid apparently observed without considering the expansion of the container is called the apparent expansion of liquid.
  9. For a given heat energy, the real expansion is always more than that of apparent expansion.
  10. If the atoms or molecules of a gas do not interact with each other, then the gas is said to be an ideal gas or a perfect gas.
  11. Ideal gas equation, also called as equation of state is \(PV = RT\). Here, R is known as universal gas constant whose value is 8.31 J mol-1K-1
Tags: Thermal Physics | Science, 10th Science : Chapter 3 : Thermal Physics
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Understanding the Fundamental Laws of Gases: Boyle's, Charles's, and Avogadro's Law

Fundamental Laws of Gases

This post provides study material, lecturing notes, and a detailed explanation of the fundamental laws governing gases in thermal physics.

Introduction to Gas Laws

The three fundamental laws which connect the relation between pressure, volume and temperature are as follows:

  1. Boyle’s Law
  2. Charles's law
  3. Avogadro's law

1. Boyle’s law:

When the temperature of a gas is kept constant, the volume of a fixed mass of gas is inversely proportional to its pressure. This is shown in Figure 3.6.

\( P \propto \frac{1}{V} \)
Figure 3.6 Variation of volume with pressure
Figure 3.6 Variation of volume with pressure

In other words, for an invariable mass of a perfect gas, at constant temperature, the product of its pressure and volume is a constant.

\( PV = \text{constant} \)

2. Charles's law (The law of volume)

Charles’s law was formulated by a French scientist Jacques Charles. According to this law, When the pressure of gas is kept constant, the volume of a gas is directly proportional to the temperature of the gas.

\( V \propto T \)

or

\( \frac{V}{T} = \text{constant} \)
Graph showing Volume is directly proportional to Temperature

3. Avogadro's law

Avogadro's law states that at constant pressure and temperature, the volume of a gas is directly proportional to number of atoms or molecules present in it.

i.e. \( V \propto n \)

(or)

\( \frac{V}{n} = \text{constant} \)
Diagram showing V/n = constant

Avogadro’s number (\(N_A\)) is the total number of atoms per mole of the substance. It is equal to \(6.023 \times 10^{23}\) /mol.

Understanding the Effect of Heat Energy: Thermal Expansion in Solids, Liquids, and Gases

EFFECT OF HEAT ENERGY

When a certain amount of heat energy is given to a substance, it will undergo one or more of the following changes:

  • Temperature of the substance rises.
  • The substance may change its state from solid to liquid or from liquid to gas.
  • The substance will expand when heated.

The rise in temperature is in proportion to the amount of heat energy supplied. It also depends on the nature and mass of the substance. About the rise in temperature and the change of state, you have studied in previous classes. In the following section, we shall discuss about the expansion of substances due to heat.

1. Expansion of Substances

When heat energy is supplied to a body, there can be an increase in the dimension of the object. This change in the dimension due to rise in temperature is called thermal expansion of the object. The expansion of liquids (e.g. mercury) can be seen when a thermometer is placed in warm water. All forms of matter (solid, liquid and gas) undergo expansion on heating.

a) Expansion in solids

When a solid is heated, the atoms gain energy and vibrate more vigorously. This results in the expansion of the solid. For a given change in temperature, the extent of expansion is smaller in solids than in liquids and gases. This is due to the rigid nature of solids.

The different types of expansion of solid are listed and explained below:

  1. Linear expansion
  2. Superficial expansion
  3. Cubical expansion
1. Linear expansion:

When a body is heated or cooled, the length of the body changes due to change in its temperature. Then the expansion is said to be linear or longitudinal expansion.

The ratio of increase in length of the body per degree rise in temperature to its unit length is called as the coefficient of linear expansion. The SI unit of Coefficient of Linear expansion is \(K^{-1}\). The value of coefficient of linear expansion is different for different materials.

Figure 3.2 Linear expansion

The equation relating the change in length and the change in temperature of a body is given below:

Equation for coefficient of linear expansion
  • \(\Delta L\) - Change in length (Final length - Original length)
  • \(L_o\) - Original length
  • \(\Delta T\) - Change in temperature (Final temperature - Initial temperature)
  • \(\alpha_L\) - Coefficient of linear expansion.
2. Superficial expansion:

If there is an increase in the area of a solid object due to heating, then the expansion is called superficial or areal expansion.

Superficial expansion is determined in terms of coefficient of superficial expansion. The ratio of increase in area of the body per degree rise in temperature to its unit area is called as coefficient of superficial expansion. Coefficient of superficial expansion is different for different materials. The SI unit of Coefficient of superficial expansion is \(K^{-1}\).

Figure 3.3 Superficial expansion

The equation relating to the change in area and the change in temperature is given below:

  • \(\Delta A\) - Change in area (Final area - Initial area)
  • \(A_o\) - Original area
  • \(\Delta T\) - Change in temperature (Final temperature - Initial temperature)
  • \(\alpha_A\) - Coefficient of superficial expansion.
3. Cubical expansion:

If there is an increase in the volume of a solid body due to heating, then the expansion is called cubical or volumetric expansion.

As in the cases of linear and areal expansion, cubical expansion is also expressed in terms of coefficient of cubical expansion. The ratio of increase in volume of the body per degree rise in temperature to its unit volume is called as coefficient of cubical expansion. This is also measured in \(K^{–1}\).

Figure 3.4 Cubical expansion

The equation relating to the change in volume and the change in temperature is given below:

Equation for coefficient of cubical expansion
  • \(\Delta V\) - Change in volume (Final volume - Initial volume)
  • \(V_o\) - Original volume
  • \(\Delta T\) - Change in temperature (Final temperature - Initial temperature)
  • \(\alpha_V\) - Coefficient of cubical expansion.

Different materials possess different coefficient of cubical expansion. Table 3.1 gives the coefficient of cubical expansion for some common materials.

Table 3.1 Coefficient of cubical expansion of some materials

b) Expansion in liquids and gases

When heated, the atoms in a liquid or gas gain energy and are forced further apart. The extent of expansion varies from substance to substance. For a given rise in temperature, a liquid will have more expansion than a solid and a gaseous substance has the highest expansion when compared with the other two. The coefficient of cubical expansion of liquid is independent of temperature whereas its value for gases depends on the temperature of gases.

When a liquid is heated, it is done by keeping the liquid in some container and supplying heat energy to the liquid through the container. The thermal energy supplied will be partly used in expanding the container and partly used in expanding the liquid. Thus, what we observe may not be the actual or real expansion of the liquid. Hence, for liquids, we can define real expansion and apparent expansion.

1) Real expansion

If a liquid is heated directly without using any container, then the expansion that you observe is termed as real expansion of the liquid.

Coefficient of real expansion is defined as the ratio of the true rise in the volume of the liquid per degree rise in temperature to its unit volume. The SI unit of coefficient of real expansion is \(K^{–1}\).

2) Apparent expansion

Heating a liquid without using a container is not possible. Thus, in practice, you can heat any liquid by pouring it in a container. A part of thermal energy is used in expanding the container and a part is used in expanding the liquid. Thus, what you observe is not the actual or real expansion of the liquid. The expansion of a liquid apparently observed without considering the expansion of the container is called the apparent expansion of the liquid.

Coefficient of apparent expansion is defined as the ratio of the apparent rise in the volume of the liquid per degree rise in temperature to its unit volume. The SI unit of coefficient of apparent expansion is \(K^{–1}\).

2. Experiment to measure real and apparent expansion of liquid

To start with, the liquid whose real and apparent expansion is to be determined is poured in a container up to a level. Mark this level as \(L_1\). Now, heat the container and the liquid using a burner as shown in the Figure 3.5.

Initially, the container receives the thermal energy and it expands. As a result, the volume of the liquid appears to have reduced. Mark this reduced level of liquid as \(L_2\).

On further heating, the thermal energy supplied to the liquid through the container results in the expansion of the liquid. Hence, the level of liquid rises to \(L_3\). Now, the difference between the levels \(L_1\) and \(L_3\) is called as apparent expansion, and the difference between the levels \(L_2\) and \(L_3\) is called real expansion. The real expansion is always more than that of apparent expansion.

Figure 3.5 Real and apparent expansion of liquid

Real expansion = \(L_3 - L_2\)

Apparent expansion = \(L_3 - L_1\)

Study Material, Lecturing Notes, Assignment, Reference, Wiki description explanation, brief detail for 10th Science : Chapter 3 : Thermal Physics : Effect of Heat Energy.

Understanding Temperature, Thermal Equilibrium, and Absolute Scale in Thermal Physics

Temperature

Introduction to Temperature

TEMPERATURE

Temperature is defined as the degree of hotness of a body. The temperature is higher for a hotter body than for a colder body. It is also be defined as the property which determines whether a body is in equilibrium or not with the surroundings. (or average kinetic enegy of the molecules). Further, temperature is the property, which determines the direction of flow of heat. It is a scalar quantity. The SI unit of temperature is kelvin (K). There are other commonly used units of temperature such as degree celsius (°C) and degree fahrenheit (°F).

1. Absolute scale (kelvin scale) of temperature

The temperature measured in relation to absolute zero using the kelvin scale is known as absolute temperature. It is also known as the thermodynamic temperature. Each unit of the thermodynamic scale of temperature is defined as the fraction of 1/273.16th part of the thermodynamic temperature of the triple point of water. A temperature difference of 1°C is equal to that of 1K. Zero Kelvin is the absolute scale of tempeture of the body.

The relation between the different types of scale of temperature:

Celsius and Kelvin: \( K = C + 273 \)

Fahrenheit and Kelvin: \( [K] = (F + 460) \times \frac{5}{9} \)

\( 0\,\text{K} = –273\,^\circ\text{C} \)

2. Thermal equilibrium

Two or more physical systems or bodies are said to be in thermal equilibrium if there is no net flow of thermal energy between the systems. Heat energy always flows from one body to the other due to a temperature difference between them. Thus, you can define thermal equilibrium in another way. If two bodies are said to be in thermal equilibrium, then, they will be at the same temperature. What will happen if two bodies at different temperatures are brought in contact with one other? There will be a transfer of heat energy from the hot body to the cold body until a thermal equilibrium is established between them. This is depicted in Figure 3.1.

Figure 3.1 Establishing thermal equilibrium

Figure 3.1 Establishing thermal equilibrium

When a cold body is placed in contact with a hot body, some thermal energy is transferred from the hot body to the cold body. As a result, there is some rise in the temperature of the cold body and decrease in the temperature of the hot body. This process will continue until these two bodies attain the same temperature.

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10th Science : Chapter 3 : Thermal Physics : Temperature

Linear Momentum: Definition, Formula, and Units | 10th Science Laws of Motion

10th Science : Chapter 1 : Laws of Motion : Introduction

Linear Momentum

LINEAR MOMENTUM

The impact of a force is more if the velocity and the mass of the body is more. To quantify the impact of a force exactly, a new physical quantity known as linear momentum is defined. The linear momentum measures the impact of a force on a body.

The product of mass and velocity of a moving body gives the magnitude of linear momentum. It acts in the direction of the velocity of the object. Linear momentum is a vector quantity.

Linear Momentum = mass × velocity

p = m v

It helps to measure the magnitude of a force. Unit of momentum in SI system is kg m s–1 and in C.G.S system its unit is g cm s-1.

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Study Material, Lecturing Notes, Assignment, Reference, Wiki description explanation, brief detail for 10th Science : Chapter 1 : Laws of Motion.