Monday, October 30, 2017

Index of all chapters

Quality solutions of all chapters are as follows:

Chapter 1
Chapter 2
Chapter 3
Chapter 4
Chapter 5
Chapter 6
Chapter 7
Chapter 8
Chapter 9
Chapter 10
Chapter 11
Chapter 12
Chapter 13
Chapter 14
Chapter 15

Sunday, November 22, 2015

WRONG PROBLEM OF HC VERMA

·         WRONG PROBLEM OF H C VERMA
H C Verma  (Part 2)  Gauss’s Law   Page # 141        Problem # 4
Q. The electric field in a region is given by E = (Eox/L) i . Find the charge contained inside a cubical volume bounded by the surfaces x = 0, x = a, y = 0, y = a, z = 0, z = a. Take Eo = 5 ×103 N/C, L = 2 cm and a = 1 cm.  
SOLUTION:
NOTE: This question has conceptual mistake.
    •  As electric field is given by the eqn. E = (Eox/L) i , it means electric field is towards positive x-axis right of y-z axis and it is towards –ve x axis  left of y-z axis. 
    • It means field lines are parallel.
    • Parallel field lines mean that field is uniform.
    • But as field depends on value of x, it can’t be uniform.
    • Hence, there is a contradiction.

    • Figure explanation.
    • Plane x = 0 corresponds to y-z plane , shown by left face in the figure.
    • Plane x = a corresponds to y-z plane , shown by right face in the figure.
    • Plane y = 0 corresponds to x-z plane , shown by bottom face in the figure.
    • Plane y = a corresponds to x-z plane , shown by top face in the figure.
    • Plane z = 0 corresponds to x-y plane , shown by back face in the figure.
    • Plane z = a corresponds to x-y plane , shown by front face in the figure.


Thursday, November 5, 2015

About this blog

HCV VERMA FULLY EXPLAINED


My aim to create solutions of hcverma from all resources. We all know that hcverma is a must must book for all iit jee aspirants. And there are different solutions available freely, but none of the solution is good enough.

 All provide solutions accurately but in case of good questions solutions are not upto the mark. So this is a platform where you get solutions from all the available resources and try to put all types of solutions. You can yourself decide which solutions you want.


 Be a follower of this blog and get quality solution of hcverma. No need to do lot of surfing and no need to try to locate best solutions. Be a part of of his blog and also comment which solution you want at the earliest. 



Which solution you want to eemove from the blog, try to locate errors in solution, also comment for alternate solutions, you can also comment and post your own solutions. 




Happy solving hcverma. Thanks very much - from Rajeev Sharma.

Sunday, September 27, 2015

52

Six particles situated at the corners of a regular hexagon of side a move at a constant speed v. Each particle maintains a direction towards the particle at the next corner. Calculate the time the particles will take to meet each other.


this question is similar to last example of hcv. please write down that example in comment box.


Consider any particle say A which moves towards B with a speed of v. But the particle B is itself moving with a speed v along BC. So movement of particle B along the AB direction will be v.cosCBG = v.cos60° =v/2.  

Now the relative speed of Particle A with respect to particle B 

= v-v/2 = v/2,     This is the effective speed with which they come closer. To travel a distance of 'a' the time taken 

= Distance/speed 

= a/(v/2) =2a/v.

It's simple, just find the component of velocity of any particle towards the center, and it won't change throughout the motion (imagine this, it's the "emotions" of physics .... Dinesh will understand the statement :P)
So, the component of the velocity towards center, you can find it easily, and then the distance between center and any particle, then just get the time= . not tough at all.....
You may want to see the solution I wrote to your problem (square one)

Note that this will happen if and only if the polygon is regular polygon and the speed of each of the particles is the same.



The time it takes is exactly 2 times the time it takes for any particle to travel the length of one side of the hexagon. If there were 4 particles in a square, the time is the same as travelling a side. Given any regular polygon, since at any time after pursuit begins, the particles are at the corners of the same regular polygon but a shrinking one, the time it takes is the same as finding the length of logarithmic spirals, which have the property of self-similarity.

Okay, if you want to prove they will, first draw a hexagon slightly smaller the first, but inside it, such that after each particle has traveled a very short distance, they're all still headed towards each other. By property of self-similarity, this can be repeated until the innermost hexagon has shrunk to a point. The paths traced out by the particles is a logarithmic spiral, which has a finite arc length from any point on it down to the center.
A shrinking hexagon indicates that the particles are getting closer to each other, because the sides are shrinking.
As a counterexample, if each particle was constrained to move only along a circular path common to all of them, then they'll never get any closer.



Hey friends i just tried to deduce a formula for such type of problems  where  is side length and  denotes the total sides of the regular polygon




Ess Kp 
11 months, 4 weeks ago
ANSWER: 
2a/v
Plz admire this image for understanding my answer... and plz consider it as a regular hexagon
img
**now, Initial separation between two particles = Side of hexagon = a
Final separation = 0
Therefore, Relative displacement between two particles = a
Particle B has a component v cos60 along particle BC (a side)
Therefore, relative velocity with which B and C approaches each other = v - vcos60 = v/2
Since, v is constant, thus time taken by these two balls to meet each other is given by
=(Relative displacement) / Relative velocity = a/(v/2) = 2a/v
So, the time taken by the particles to meet each other = 2a/v
In reality each particle will follow a curved path and eventually meet at the center of the hexagon.*
o

51

Suppose A and B in the previous problem change their positions in such a way that the line joining them becomes perpendicular to the direction of wind while maintaining the separation x. What will be the time lag B finds between seeing and hearing the drum beating by A ?


As seen in above diagram the resultant velocity of sound will be along AB and its magnitude AE can be calculated from the right angled triangle ACE.  

AE²=AC²-CE²  = v²-u²  

AE = √(v²-u²)   

So the time lag B finds between seeing and hearing the drum beating by A 

= Distance AB /velocity AE 

= x/√(v²-u²)