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Payal Gupta

Contributor-Level 10

13.31 Amount of Electric power to be generated, P = 200000 MW

10% of which to be obtained from nuclear power.

Hence, amount of nuclear power = 10% of 2 * 10 5  MW = 2 * 10 4 MW = 2 * 10 4 * 10 6  J/s

= 2 * 10 4 * 10 6 * 60 * 60 * 24 * 365  J/y = 6.3072 * 10 17 J/y

Heat energy release per fission of a U 235  nucleus, E = 200 MeV

Efficiency of a reactor = 25%

So the amount of electrical energy converted from heat energy per fission = 25% of 200 MeV = 50 MeV

= 50 * 10 6 eV = 50 * 10 6 * 1.6 * 10 - 19 J = 8 * 10 - 12  J

Therefore, number of atoms required per year = 6.3072 * 10 17 8 * 10 - 12  = 7.884 * 10 28

1 mole of U 235  = 235 gm of U 235  contains 6.023 * 10 23 atoms

Hence the mass of 7.884 * 10 28 a t o m s  =235*10-36.023*1023 * 7.884 *1028 = 30.76 *103 kg

Hence, the Urani

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Payal Gupta

Contributor-Level 10

13.30 Amount of hydrogen, m = 1 kg = 1000 g

1 mole of hydrogen, i.e. 1 g of hydrogen ( H ) 1 1 contains 6.023 * 10 23  atoms

1 kg of hydrogen contains = 1000 * 6.023 * 10 23  atoms = 6.023 * 10 26 atoms

Within Sun, four ( H ) 1 1  nuclei combine and forms 1 H e 2 4  nucleus. In this process 26 MeV of energy is released.

Hence the energy released from fusion of 1 kg of H 1 1  is:

E 1  = 6.023 * 10 26 * 26 4  MeV = 3.91495 * 10 27 MeV

Amount of U 92 235 , m = 1 kg = 1000 g

1 mole of U 92 235 , i.e. 235 g of U 92 235  contains 6.023 * 10 23 atoms

1 kg of  U 92 235 contains = 1000 235 *  6.023 * 10 23 atoms = 2.563 * 10 24  atoms

It is known that the amount of energy released in the fission of 1 atom of U 92 235  is 200

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Payal Gupta

Contributor-Level 10

13.29 It can be observed from the given γ - decay diagram that γ 1 decays from 1.088 MeV energy level to the 0 MeV energy level.

Hence the energy corresponding to  decay is given as:

 = 1.088 – 0 = 1.088 MeV = 1.088 * 10 6  eV = 1.088 * 10 6 * 1.6 * 10 - 19 J

= 1.7408 * 10 - 13 J

We know, E 1 = h ν 1 , where

ν 1 = Frequency of radiation radiated by γ 1  decay

h = P l a n c k ' s c o n s t a n t = 6.6 * 10 - 34 Js

Hence,  ν 1 = E 1 h  = 1.7408 * 10 - 13 6.6 * 10 - 34  = 2.637 * 10 20 Hz

It can be observed from the given γ - decay diagram that γ 2 decays from 0.412 MeV energy level to the 0 MeV energy level.

Hence the energy corresponding to γ 2  decay is given as:

E 2 = 0.412 – 0 = 0.412 MeV = 0.412 * 10 6  eV = 0.412 * 10 6 * 1.6 * 10 - 19  J

= 6.592 * 10 - 14 J

W

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8 months ago

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alok kumar singh

Contributor-Level 10

Ans.1.12

(a) Charge on sphere A, qA = 6.5 *10-7 C

Charge on sphere B, qB = 6.5*10-7 C

Distance between the spheres, r = 50 cm = 0.5 m

Force of repulsion between two spheres

F = 14??0 *q1q2r2 , where ?0= Permittivity of free space = 8.854*10-12 
  C2N-1m-2Therefore, F =  14*?*8.854*10-12 *6.5*10-7*6.5*10-70.52N = 0.0152 N = 1.52  *10-2N

(b) Charge on sphere A, qA = 2 *6.5  *10-7C = 1.3 *10-6C

Charge on sphere B, qB = 2 * 6.5 *10-7C = 1.3 *10-6C

Distance between the spheres, r =  = 25 cm = 0.25 m

Force of repulsion between two spheres

F =  14??0 *q1q2r2, where ?0 = Permittivity of free space = 8.854  *10-12 C2N-1m-2Therefore, F = 
 14*?*8.854*10-12 *1.3*10-6*1.3*10-60.252N = 0.243 N

New question posted

8 months ago

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New answer posted

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Payal Gupta

Contributor-Level 10

13.25 Half life of P 15 32 , T 1 / 2 = 14.3 days

Half life of P 15 33 , T 1 / 2  = 25.3days and P 15 33  decay is 10% of the total amount of decay

The source has initially 10 % of P 15 33 nucleus and 90% of P 15 32  nucleus

Suppose after t days, the source has 10% of P 15 32  nucleus and 90% of P 15 33  nucleus

Initially:

Number of P 15 33 nucleus = N

Number of P 15 32  nucleus = 9N

 

Finally:

Number of P 15 33 nucleus = 9N'

Number of P 15 32  nucleus = N'

For P 15 32 nucleus, the number ratio, N ' 9 N  = 1 2 t / T 1 / 2

N' = 9N ( 2 ) - t / 14.3 …………….(1)

 

For P 15 33  nucleus, the number ratio, 9 N ' N = 1 2 t / T 1 / 2

9N' = N ( 2 ) - t / 25.3  …………….(2)

 

On dividing equation (1) by equation (2), we get:

1 9 = 9 * 2 ( t 25.3 - t 14.3 )

1 81  = 2 ( - 11 t 25.3 * 14.3 )

Taking l

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Payal Gupta

Contributor-Level 10

13.23 Average atomic mass of magnesium, m = 24.312 u

Mass of magnesium isotope Mg1224 ,m1= 23.98504u

Mass of magnesium isotope  Mg1225 ,m2= 24.98584u

Mass of magnesium isotope  Mg1226 ,m3= 25.98259u

Let the abundance of magnesium isotope  Mg1224 be η1 = 78.99 %

Let the abundance of magnesium isotope  Mg1225 be η2= x %

Therefore, the abundance of magnesium isotope  Mg1226 be η3= (100 - 78.99 - x) %

= (21.01 – x)%

The average atomic mass can be expressed as:

m = m1η1+m2η2+m3η3η1+η2+η3 = 23.98504*78.99+24.98584x+25.98259(21.01-x)100 = 1894.578+24.98584x+545.894-25.98259x100=2440.472-0.99675x100

24.312 = 2440.472-0.99675x100

x = 9.3%

Therefore the abundance of M g 12 25 is 9.3% and the abundance of Mg1226 is (21.01 – 9.3)11.71%

New answer posted

8 months ago

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P
Payal Gupta

Contributor-Level 10

13.22 Let the amount on energy released during the electron capture process be Q1 . The nuclear reaction can be written as:

 e++ XZA Y + v z - 1 A + Q 1 …………………….(1)

Let the amount of energy released during the positron capture process be Q2. The nuclear reaction can be written as:

 XZA Y+e++vz-1A +Q2 …………………….(2)

Let us assume

m N X Z A = Nuclear mass of X Z A

m N X Z A = Atomic mass of X Z A

m N Y Z - 1 A = Nuclear mass of Y Z - 1 A

m N Y Z - 1 A = Atomic mass of Y Z - 1 A

m e = mass of the electron

c = speed of light

 

Q-value of the electron capture reaction is given as:


Q1 = [ mNXZA+me-mNYZ-1A]c2

= [ mXZA-Zme+me-mYZ-1A+(Z-1)me]c2

= [mXZA-mYZ-1A]c2  ………………….(3)

Q-value of the positron capture reaction is given as:

Q2 = [ mNXZA-mNYZ-1A-me]c2

= [

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New question posted

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New answer posted

8 months ago

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P
Payal Gupta

Contributor-Level 10

13.21 We have the expression for nuclear radius as:

R = R0A1/3

Where R0 = constant

A = mass number of nucleus

Let m be the average mass of the nucleus, hence mass of the nucleus = mA

Nuclear matter density ρ can be written as

 ρ=MassofthenucleusVolumeofthenucleus = mA43πR3 = 3mA4π(R0A13)3 = 3mA4πR03A = 3 m 4 π R 0 3

Hence, the nuclear mass density is independent of A. It is nearly constant

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