Get 2 FREE Instant-Explanations on Filo with code FILOAPP

Home

Physics Part-II

Nuclei

From the relation R = R_0A^{1}{3} , where R_0 is a constant an

Physics Part-II

Class 12

NCERT

Chapter 1: Ray Optics and Optical Instruments

41 questions

Chapter 2: Wave Optics

30 questions

Chapter 3: Dual Nature of Radiation and Matter

44 questions

Chapter 4: Atoms

23 questions

Chapter 5: Nuclei

38 questions

Calculate the height of the potential barrier for a head on collision of two deuterons.

From the relation R =

R_{0} A^{\frac{1}{3}}

, where

R_{0}

is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).

For the

β^{+}

(positron) emission from a nucleus, there is another competing process known as electron capture (electron from an inner orbit, say, the K shell, is captured by the nucleus and a neutrino is emitted).

e^{+} +_{Z}^{A} X \to_{Z - 1}^{A} Y + v

Show that if

β^{+}

emission is energetically allowed, electron capture is necessarily allowed but not vice versa.

View all question

Chapter 6: Semiconductor Electronics: Materials, Devices and Simple Circuits

25 questions

Question

Easy

Solving time: 4 mins

From the relation R = $R_{0} A^{\frac{1}{3}}$ , where $R_{0}$ is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).

Name: Video solution 1: [Solved] From the relation R = R0A31 , where R0 is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A). - Physics Part-II
Uploaded: 2022-03-21T08:36:42.000Z
Duration: 6 min
Description: Video solution 1: [Solved] From the relation R = R0A31 , where R0 is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A). - Physics Part-II

Views: 5,487 students

Updated on: Mar 21, 2022

Book:

Physics Part-II (NCERT)

Found 8 tutors discussing this question

Charlotte Discussed

From the relation R =

R_{0} A^{\frac{1}{3}}

, where

R_{0}

is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).

7 mins ago

Discuss this question LIVE

7 mins ago

Text solutionVerified

Density of nuclear matter

=

Mass of nucleus/Volume of nucleus

= \frac{A}{\frac{4}{3} π R ^{3}}

= \frac{A}{\frac{4}{3} π ( R _{0} A ^{1/3} ) ^{3}} = \frac{1}{\frac{4}{3} π R _{0}^{3}} = co n s t an t

Was this solution helpful?

Report

Filo tutor solutions (1)

Learn from their 1-to-1 discussion with Filo tutors.

6 mins

Uploaded on: 3/21/2022

Ask your question, on a video call with tutor

Connect instantly with this tutor

Connect now

Taught by

Rajkumar Sain

Total classes on Filo by this tutor - 1,939

Teaches : Physics

Connect instantly with this tutor

Connect now

Was this solution helpful?

Report

One destination for complete JEE/NEET preparation

One destination to cover all your homework and assignment needs

Learn Practice Revision Succeed

Instant 1:1 help, 24x7

60, 000+ Expert tutors

Textbook solutions

Big idea maths, McGraw-Hill Education etc

Essay review

Get expert feedback on your essay

Schedule classes

High dosage tutoring from Dedicated 3 experts

Trusted by 4 million+ students

Practice more questions from Physics Part-II (NCERT)

Calculate the height of the potential barrier for a head on collision of two deuterons.

From the relation R =

R_{0} A^{\frac{1}{3}}

, where

R_{0}

is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).

For the

β^{+}

e^{+} +_{Z}^{A} X \to_{Z - 1}^{A} Y + v

Show that if

β^{+}

emission is energetically allowed, electron capture is necessarily allowed but not vice versa.

View all

Stuck on the question or explanation?

Connect with our Physics tutors online and get step by step solution of this question.

231 students are taking LIVE classes

Question Text	From the relation R = $R_{0} A^{\frac{1}{3}}$ , where $R_{0}$ is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).
Updated On	Mar 21, 2022
Topic	Nuclei
Subject	Physics
Class	Class 12
Answer Type	Text solution:1 Video solution: 1
Upvotes	178
Avg. Video Duration	6 min

From the relation R = $R_{0} A^{\frac{1}{3}}$ , where $R_{0}$ is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).

Text solutionVerified

Filo tutor solutions (1)

Practice more questions from Physics Part-II (NCERT)

Practice questions from Physics Part-II (NCERT)

Practice more questions from Nuclei

Practice questions on similar concepts asked by Filo students

From the relation R = R0​A31​ , where R0​ is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).

Text solutionVerified

Filo tutor solutions (1)

Practice more questions from Physics Part-II (NCERT)

Practice questions from Physics Part-II (NCERT)

Practice more questions from Nuclei

Practice questions on similar concepts asked by Filo students

Related books for questions on Nuclei

From the relation R = $R_{0} A^{\frac{1}{3}}$ , where $R_{0}$ is a constant and A is the mass number of a nucleus, show that the nuclear matter density is nearly constant (i.e. independent of A).