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Physics Blog
All about Physics

We are starting a new segment on the blog where we recommend one or two books in Math or Physics that everyone can read.

And this month it is *: A Mathematician’s Apology* by G.H.Hardy which is available for free to download here and here

You are absolutely welcome to share your comments and reviews here once you are done. Also, if you would like us to check a book out, do let us know too!

Have a good one!

One of my professors was asked the same question and let me paraphrase his response:

You give up on intuition when it gives up on you.

One of the many reasons why most of physics is deeply mathematical is because our intuition alone is unable to explain all the results that we observe in nature and when that happens, we rely on mathematical theories to shed light on the nature of reality

** The reason why this is awesome is because one does need to worry about the unit vectors in the r and theta directions, which makes the algebra so much more simpler

The Buddhabrot is an interesting fractal rendering technique for displaying the Mandelbrot Set.

Its name reflects its pareidolic resemblance to classical depictions of Gautama Buddha, seated in a meditation pose with a forehead mark (

tikka) and traditional topknot (ushnisha).

* Read more interesting things about Buddhabrot and Nebulabrot here

** Pareidolia is a psychological phenomenon in which the mind responds to an image or a sound, by perceiving a familiar pattern where none exists. Check out more examples of pareidolia here

If one remembers this particular episode from the popular sitcom ‘Friends’ where Ross is trying to carry a sofa to his apartment, it seems that moving a sofa up the stairs is ridiculously hard.

But life shouldn’t be that hard now should it?

The mathematician Leo Moser posed in 1966 the following curious mathematical problem:

whatThis question became known as the

is the shape of largest area in the plane that can be moved around a

right-angled corner in a two-dimensional hallway of width 1?moving sofa problem, and is still unsolved fifty years after it was first asked.

The most common shape to move around a tight right angled corner is a square.

And another common shape that would satisfy this criterion is a semi-circle.

But

what is the largest area that can be moved around?

Well, it has been

conjectured that the shape with the largest area that one can move around a corner is known as “Gerver’s

sofa”. And it looks like so:

This

sofa would only be effective for right handed turns. One can clearly

see that if we were to turn left somewhere we would in kind of tough

situation.

Prof.Romik from the University of California has

proposed this shape popularly know as Romik’s ambidextrous sofa that

solves this problem.

Although Prof.Romik’s sofa may/may not be the not the optimal solution, it is definitely is a breakthrough since this can pave the way for more complex ideas in mathematical analysis and sofa design.

Once when lecturing in class Lord Kelvin used

the word ‘mathematician’ and then interrupting himself asked his class:

’Do you know what a mathematician is?’Stepping to his blackboard he

wrote upon it the above equation.Then putting his finger on what he had written, he turned to

his class and said,‘A mathematician is one to whom that is as obvious’

as that twice two makes four is to you.

Woah… The backlash that Lord Kelvin got after this post was just phenomenal.

There are many ways to obtain this integral *(click here to know about other methods)* , but here are two interesting ways to arrive at the Gaussian Integral which you *may/may not have seen and may/may not be easy to follow.*

If you know about factorials (5!= 5.4.3.2.1), you know that they make sense only for integers.

But Gamma function

extends this to non-integers values. This integral form allows you to

calculate factorial values such as (½)!, (¾)! and so on.

The same can be used to evaluate the Gaussian Integral as follows:

In this technique known as ‘Differentiating under the integral sign’, you choose an integral whose boundary values are easy integrals to evaluate.

Here I(0) and I(∞); and differentiate with respect to a parameter β instead of the variable x to obtain the result.