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8 months ago

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Payal Gupta

Contributor-Level 10

13.11 Length of the narrow bore, L = 1 m = 100 cm

Length of the mercury thread, l = 76 cm

Length of the air column between mercury and the closed end, lo  = 15 cm

Since the bore is held vertically in air with the open end at the bottom, the mercury length that occupies the air space is 100 – (76 + 15) = 9 cm

Hence, total length of the air column = 15 + 9 = 24 cm

Let h cm of mercury flow out as a result of atmospheric pressure.

Length of the air column in the bore = 24 + h cm

Length of the mercury column = 76 – h cm

Initial pressure,  P1 = 76 cm of mercury

Initial volume, V1= 15 cm3

Final pressure, P2 = 76 – (76 – h) = h cm

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8 months ago

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Payal Gupta

Contributor-Level 10

13.10 Pressure inside the cylinder containing nitrogen, P = 2.0 atm = 2 *1.013*105 Pa

Temperature inside the cylinder, T = 17 ?=290K

Radius of nitrogen molecule, r = 1.0 Å = 1 *10-10 m

Diameter of nitrogen molecule, d = 2 *10-10 m

Molecular mass of nitrogen molecule, M = 28 u = 28 g (assume) = 28 *10-3 kg

The root means square speed of nitrogen is given by the relation

R is the universal gas constant = 8.314 J/mole/K

Hence 

The mean free path l is given by

l ?=kT?2?d2P where k = Boltzmann constant = 1.38*10-23 kg-m2s-2K-1 

l?=1.38*10-23*290?2?(2*10-10)2*2*1.013*105= 1.11*10-7  m

Collision frequency = Vrmsl? = 508.261.11*10-7= 4.57 109 /s

Collision time, T = dVrms  =2*10-10508.26S= 3.93 *10-13 s

T

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New answer posted

8 months ago

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Payal Gupta

Contributor-Level 10

13.9 Temperature of the helium atom, THe = – 20 °C = 253 K and temperature of argon atom be = TAr

Atomic mass of helium, MHe = 4.0 u

Atomic mass of Argon, MAr = 39.9 u

Let VrmsAr be the rms speed of Argon and VrmsHe be the rms speed of Helium

From the relation of Vrms=3kTM we get

rms speed of Argon, VrmsAr=3kTArMAr

rms speed of Helium, VrmsHe=3kTHeMHe

Since both the speeds are equal, we get

3kTArMAr = 3kTHeMHe or TArMAr = THeMHe or TAr = THe*MArMHe = 253*39.94 = 2523.675 K = 2.523 *103 K

New answer posted

8 months ago

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Pallavi Pathak

Contributor-Level 10

Diffraction leads to the formation of patterns of varying intensity. When around obstacles, waves bend and spread through the narrow opening, it is called diffraction. The interference results in a new wave pattern and involves the superposition of two or more coherent waves. Both these phenomena produce patterns of light and dark regions; the interference results from the combination of multiple waves and the diffraction arises from a single wave interacting with an aperture or obstacle. When the size of the aperture or obstacle is comparable to the wavelength of the wave, diffraction patterns are typically observed.

New answer posted

8 months ago

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Payal Gupta

Contributor-Level 10

13.8  (a) According to Avogadro's law, the three vessels will contain an equal number of the respective molecules. This number is equal to Avogadro's number, N = 6.023 *1023

(b) The root mean square speed ( Vrms) of a gas of mass m and temperature T is given by the relation Vrms=3kTm . Where k is Boltzmann constant. For the given gases, k and T are constants. Hence Vrms depends only on the mass of the atoms

Therefore, the root mean square speed of the molecules in the three cases is not the same. Among Neon, Chlorine and Uranium hexafluoride, the mass of the neon is the smallest, so Neon will have the highest root mean square sp

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8 months ago

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Pallavi Pathak

Contributor-Level 10

A coherent light source in Young's Double Slit Experiment illuminates two closely spaced slits, and produces two overlapping light waves. The interference of these waves constructively or destructively based on their phase difference lead to a pattern of bright and dark fringes on a screen, When the path difference is an integral multiple of the wavelength, it is constructive interference (bright fringes) and when the path difference is an odd multiple of half the wavelength, it is destructive interference (dark fringes). Through observable interference patterns, Young's Double Slit Experiment, shows the wave nature of light.

New answer posted

8 months ago

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P
Payal Gupta

Contributor-Level 10

13.7 (i) At room temperature, T = 27 ? = 300 K

kB is Boltzmann constant = 1.38 *10-23 m2kgs-2K-1

Average thermal energy = 32kBT = 3*1.38*10-23*3002 = 6.21 *10-21 J

Hence, the average thermal energy of a helium atom at room temperature is 6.21 *10-21 J

(ii) On the surface of the Sun, T = 6000 K

Hence average thermal energy = 32kBT = 3*1.38*10-23*60002 = 1.242 *10-19 J

Hence, the average thermal energy of a helium atom on the surface of the Sun is 1.242 *10-19 J

(iii) Inside the core of a star, T = 107 K

Hence average thermal energy = 32kBT = 3*1.38*10-23*1072 = 2.07 *10-16 J

Hence, the average thermal energy of a helium atom

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8 months ago

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Vishal Baghel

Contributor-Level 10

4.21:

(a) Velocity , v? = 10.0 ? m/s

Acceleration, a? = (8.0 ? + 2.0 ?) m s-2

We know a? = dv?dt = 8.0 ? + 2.0 ?

dv? = (8.0 ? + 2.0 ?)dt

Integrating both sides we get v? (t) = 8.0t ? + 2.0t ? + u? ,

Where, u?= velocity vector of the particle at t =0

v?= velocity vector of the particle at time t

But v? = drdt

dr? = v? dt

= (8.0t ? + 2.0t ? + u? )dt

Integrating both sides with the condition at t = 0, r =0 and at t =t, r = r

r?= u? t + ½ * 8.0 t2 ? + ½ * 2.0 * t2 ? = u? t + 4.0 t2 ? + t2 ?

Substituting the value of u? , we g

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New answer posted

8 months ago

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Payal Gupta

Contributor-Level 10

13.6 Volume of the room, V = 25.0 m3

Temperature of the room, T = 27 ?  = 300 K

Pressure of the room, P = 1 atm = 1 * 1.013 *105 Pa

The ideal gas equation relating to pressure (P), volume (V) and absolute temperature (T) can be written as

PV = kB NT, where kB is Boltzmann constant = 1.38 *10-23 m2kgs-2K-1

N is the number of air molecules in the room.

N = PVkBT = 1*1.013*105*251.38*10-23*300 = 6.117 *1026

New answer posted

8 months ago

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Pallavi Pathak

Contributor-Level 10

According to Chapter 10 Physics Class 12, the Huygens' Principle in wave optics states that every point on a wave front spreads out in all directions at the speed of the wave, and these act as a source of secondary wavelets. According to this principle, all new wave front is the tangent to these secondary wavelets. The principle holds significance when it comes to explaining phenomena like refraction and reflection of light. It is instrumental in understanding the behavior of light in various media and provides a geometric method to determine the propagation of wave fronts. The Huygens' Principle lays the foundation for the wave theory

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