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Physics Test-13

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Physics Test-13
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  • Question 1
    4 / -1

    Which of the following is correct for entropy of an isolated system?

    Solution

    It can never decrease is correctfor entropy of an isolated system,

    Second law of thermodynamics:

    The entropy of an isolated system not in equilibrium will tend to increase over time, approaching a maximum value at equilibrium.

    In other words, The second law of thermodynamics states that the total entropy of an isolated system always increases over time, or remains constant in ideal cases where the system is in a steady-state or undergoing a reversible process. This increase in entropy accounts for the irreversibility of natural processes.

    The second law gives the definition of entropy term.

    \(\Delta S=\frac{\Delta Q}{T}\)

    Where \(\Delta S\) is the entropy change, \(\Delta Q\) is the energy change and \(T\) is the temperature.

    Isolated system: The system which doesn't interact with the surrounding is called isolated system. The universe is assumed as an isolated system.

    According to the second law of thermodynamics, the entropy of an isolated system increases with time It can never decrease.

    Since the universe is assumed as an isolated system and the entropy of an isolated system always increases with time.

    As the entropy of an isolated system increases always, so the entropy change of an isolated system can never be negative.

  • Question 2
    4 / -1

    A porter lifts a luggage of \(15\) kg from the ground and puts it on his head \(1.5\) m above the ground. Calculate the work done by him on the luggage.

    Solution

    Given,

    Mass of luggage, \((m)=15\) kg

    Displacement \((s)=1.5\) m

    As we know,

    Work done, \((W)=F \times s=mg \times s\)

    \(=15\) kg \(\times 10 \) ms\(^{-2} \times 1.5\) m

    \(=225\) kg ms\(^{-2}\) m

    \(=225\) Nm

    \(=225\) J

  • Question 3
    4 / -1

    A body of M.I. of \(3 \mathrm{~kg}-\mathrm{m}^{2}\), rotating with an angular velocity of \(2 \mathrm{rad} / \mathrm{s}\), has the same K.E. as a mass of \(12 \mathrm{~kg}\) moving with a velocity of:

    Solution
    Given:
    Moment of inertia \((I)=3 \mathrm{~kg}-\mathrm{m}^{2}\)
    Angular Velocity \((\omega)=2 \mathrm{rad} / \mathrm{s}\)
    Mass \((\mathrm{m})=12 \mathrm{~kg}\)
    To Find velocity (v)
    The velocity is given as,
    \(\frac{1}{2} \mathrm{I} \omega^{2}=\frac{1}{2} \mathrm{mv}^{2}\)
    \(\frac{1}{2} \times 3(2)^{2}=\frac{1}{2} \times 12 \times \mathrm{v}^{2}\)
    \(\mathrm{v}=1 \mathrm{~m} / \mathrm{s}\)
    Thus, the speed of the body is \(1 \mathrm{~m} / \mathrm{s}\).
  • Question 4
    4 / -1

    Chemical effect of current is not used in:

    Solution

    Chemical effect of current is not used in electrotyping.

    In glowing of a bulb, electrical energy charges to light energy. Electrolysis refers to chemical decomposition produced by passing an electric current through a liquid or solution containing ions.

  • Question 5
    4 / -1

    Wavelength of X-ray is of the order:

    Solution

    Since, 1 nm = 10-9 m

    The wavelength (λ) range of X-rays: 0.01 nm to 10 nm

    So λ = (0.01 × 10-9 ) m to (10 × 10-9 ) m = 10-11 m to 10-8 m

    Thus, the Wavelength of the X-ray is of the order: 10-10 m.

  • Question 6
    4 / -1

    _____________ diode is designed to work under breakdown region.

    Solution

    Zener diodeis designed to work under breakdown region.

    A Zener diode is a special type of diode designed to reliably allow current to flow "backwards" when a certain set reverse voltage, known as the Zener voltage, is reached.

    Zener diodes are widely used in electronic equipment of all kinds and are one of the basic building blocks of electronic circuits. They are used to generate low-power stabilized supply rails from a higher voltage and to provide reference voltages for circuits, especially stabilized power supplies. They are also used to protect circuits from overvoltage, especially electrostatic discharge (ESD).

  • Question 7
    4 / -1

    The force per unit length is 10-3 N on the two current-carrying wires of equal length that are separated by a distance of 2 m and placed parallel to each other. If the current in both the wires is doubled and the distance between the wires is halved, then what will be the force per unit length on the wire?

    Solution

    Given: Initially force per unit length on the wires \(= f _{ ab }= f _{ ba }= f =10^{-3}\) N and \(d =2\) m

    If two current carrying long wires \(A\) and \(B\) are separated by a very small distance and placed parallel to each other. Then the force per unit length on wire \(A\) and wire \(B\) is given as,

    \(f_{a b}=f_{b a}=f=\frac{\mu_{o} I_{a} I_{b}}{2 \pi d}\)

    Where, \(I _{ a }=\) current in the wire \(A , I _{ b }=\) current in the wire \(B\), and \(d =\) distance between the wires

    If the current in both the wires is doubled,

    \(I_{a}^{\prime}=2 I_{a}\)

    \(\Rightarrow I_{b}^{\prime}=2 I_{b}\)

    And the distance between the wires is halved, so,

    \(d^{\prime}=\frac{d}{2}\)

    So, when the current in both the wires is doubled and the distance between the wires is halved, the new force per unit length on wire A and wire B will be,

    \(f_{a b}^{\prime}=f_{b a}^{\prime}=f^{\prime}=\frac{\mu_{o} I_{a}^{\prime} I_{b}^{\prime}}{2 \pi d^{\prime}}\)

    \(\Rightarrow f^{\prime}=2 \times \frac{\mu_{o} \times 2 I_{a} \times 2 I_{b}}{2 \pi d}\)

    \(\Rightarrow f^{\prime}=8 \times \frac{\mu_{o} I_{a} I_{b}}{2 \pi d}\)

    \(\Rightarrow f ^{\prime}=8 f\)

    \(\Rightarrow f ^{\prime}=8 \times 10^{-3}\) N

  • Question 8
    4 / -1

    Rain drops are spherical because of _______________.

    Solution

    A small liquid drop has a spherical shape, as due to surface tension the liquid surface tries to have the minimum surface area and for a given volume, the sphere has a minimum surface area.

  • Question 9
    4 / -1

    What is the correct expression for Binding energy of a satellite.

    Solution

    Binding Energy can be defined as the minimum energy required to be supplied to it order to free the satellite from the gravitational influence of the planet. (in order to take the satellite from the orbit to as point if infinity.)

    Consider a satellite revolving around a planet with speed V at a distance r.


    Kinetic Energy \(=\frac{1}{2} \mathrm{~m}_{\mathrm{s}} \mathrm{V}^{2} \)

    Potential Energy \(=\frac{\mathrm{GM}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{\mathrm{r}} \)

    \(\mathrm{E}=\frac{\mathrm{GM}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{\mathrm{r}^{2}}=\frac{\mathrm{msV}^{2}}{\mathrm{r}} \)

    \(\Rightarrow \mathrm{m}_{3} \mathrm{~V}^{2}=\frac{4 \mathrm{M}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{\mathrm{r}} \)

    Kinetic Energy \(=\frac{1}{2} \frac{\mathrm{Gm}_{\mathrm{s}} \mathrm{M}_{\mathrm{p}}}{\mathrm{r}}\)

    Total Energy\(=\mathrm{K} \cdot \mathrm{E}+\mathrm{P} \cdot \mathrm{E}=\frac{1}{2} \frac{\mathrm{GM}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{\mathrm{r}}-\frac{\mathrm{GM}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{\mathrm{r}}\)

    Total Energy \(=\frac{-\mathrm{GM}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{2 \mathrm{r}} \)

    Binding Energy \(+\) Total Energy = 0 (at infinite TE= 0)

    Binding Energy \(=\frac{\mathrm{GP}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{2 \mathrm{r}}=0\)

    Binding Energy \(=\frac{\mathrm{GM}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{2 \mathrm{r}}\)

    So Binding energy of satellite \(\mathrm{G}\) of man \(\mathrm{m}_{\mathrm{s}}\) revolving around a planet of \(\operatorname{man} \mathrm{M}_{\mathrm{p}}\) in a radius \(\mathrm{r}\) \(\text { is }=\frac{\mathrm{GM}_{\mathrm{p}} \mathrm{m}_{\mathrm{s}}}{2 \mathrm{r}}\)

  • Question 10
    4 / -1

    Two particles execute SHM of the same amplitude and frequency along the same straight line. If they pass one another when going in opposite directions, each time their displacement is half their amplitude, the phase difference between them is:

    Solution

    We know that:The equation for SHM is:

    \(\mathrm{y}=\operatorname{Asin}(\omega+\phi)\)

    As the displacement is half of the amplitudes so:\(\left(\mathrm{y}=\frac{\mathrm{A}}{2}\right)\)

    or \(\frac{\mathrm{A}}{2}=\mathrm{A} \sin (\omega \mathrm{t}+\)\(\phi) \)

    \((\omega t+\phi)=\frac{1}{2} \)

    \(\therefore \omega \mathrm{t}+\phi=30^{\circ} \text { or } 150^{\circ}\)

    Since the two particles are going in opposite directions, the phase of one is \(30^{\circ}\) and that of the other \(150^{\circ} .\)

    So the phase difference between the two particles:

    \(=150^{\circ}-30^{\circ}\)

    \(=120^{\circ}\)

    \(=\frac{2 \pi}{3}\)

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