States of Matter

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Payal Gupta

Contributor-Level 10

5.25.  (a) Other than attractive forces, molecules also exert repulsive forces on one another. When two molecules are brought into close contact with each other, the repulsion between the electron clouds and that between the nuclei of two molecules comes into play. Magnitude of the repulsion rises very rapidly as the distance separating the molecules decreases. This is the reason that liquids and solids are hard to compress. In these states molecules are already in close contact; therefore, they resist further compression; as that would result in the increase of repulsive interactions.

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Payal Gupta

Contributor-Level 10

5.24.  (b) Viscosity of liquids decreases as the temperature rises because at high temperature molecules have high kinetic energy and can overcome the intermolecular forces to slip past one another between the layers.

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Payal Gupta

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5.23.  (a) The dipole-dipole interaction between two HCl molecules is stronger than the London forces but is weaker than ion-ion interaction because only partial charges are involved.

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Payal Gupta

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5.22. Higher the critical temperature, more easily the gas can be liquefied, i.e., greater are the intermolecular forces of attraction. Hence, CO2 has stronger intermolecular forces than CH4.

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Payal Gupta

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5.21. At -273°C, volume of the gas becomes equal to zero, i.e., the gas ceases to exist.

 

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Payal Gupta

Contributor-Level 10

5.20. SI unit of pressure, P = Nm-2

SI unit of volume = m3

Si unit of temperature, T = K

SI unit of number of moles, n = mol

Thus, SI unit of pV2T2/n = (Nm-2) (m3)2 (K) 2mol = Nm4K2mol-1

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Payal Gupta

Contributor-Level 10

5.19. As the mixture Hand O2 contains 20% by weight of dihydrogen, therefore,

If H2 = 20g, then O2 = 80g

No. of moles of H2 = 20/2 = 10 moles

No. of moles of O2 = 80/32 = 2.5 moles

Partial pressure of H2 = [No. of moles of H2/ (No. of moles of H2 + No. of moles of O2)] x

Ptotal= [10 (10 + 2.5)] x 1 = 0.8 bar

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Payal Gupta

Contributor-Level 10

5.18. Given, P1 = P2 and V1 = V2

We know that P1V1 = P2V2

Or,                n1RT1 = n2RT2

i.e.,                  n1T1 = n2T2

 Substituting n = w/M, we get

(W1/M1) x T1 = (W2/M2) x T2

(2.9/M1) x (95 + 273) = (0.184/2) x (17 + 273)

M1 = (2.9 x 368 x 2) / (0.184 x 290) = 40 g mol-1

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Payal Gupta

Contributor-Level 10

5.17. No. of moles of CO2 = Given mass of CO2 / Molar mass

                                           = 8.8g / 44g mol-1 = 0.2 mol

Pressure of CO2 = 1 bar

RR = 0.083 bar dm3 K–1 mol–1

T = 273 + 31.1 K = 304.1 K

According to ideal gas equation,

PV = nRT

Therefore, V = nRT/P

                      = (0.2 x 0.083 x 304.1) / 1 bar = 5.048 L

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Payal Gupta

Contributor-Level 10

5.16. Radius of the balloon = 10 m

Therefore, volume of the balloon = (4/3)? r3 = (4/3) x (22/7) x (10 m)3

= 4190.5 m3

Volume of He filled at 1.66 bar and 27 °C = 4290.5 m3

To calculate the mass of He,

PV = nRT = (w/M) RT, where M is molar mass of He i.e. 4 g per mole or 4 x 10-3 kg mol-1

=> w =  [ (4 x 10-3 kg mol-1) (1.66 bar) (4190.5 m3)] / [ (0.083 bar dm3 K-1 mol-1) (300K)]

         = 1117.5 kg

Total mass of the balloon along with He = 100 + 1117.5 = 1217.5 kg

Maximum mass of the air that can be displaced by balloon to go up = volume x density

= 4190.5 m3 x 1.2 kg m-3 = 5028.6 kg

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