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07:15
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2 hours later…
09:30
@JohnRennie: Hi sir :-)
@GuruVishnu hi
in The h Bar, 2 mins ago, by Guru Vishnu
As per the new Cartesian sign convention in optics, is it ok to determine the nature of object or image based on the signs of object and image distance?
Or in other words; is positive value of something always virtual and negative value always real for object and the exact opposite for images, sir?
Yes, the whole point of a sign convention is that it enables you to work out the details of the system you are studying.
+ object distance - virtual object
- object distance - real object
+ image distance - real image
- image distance - virtual image
@GuruVishnu That's true for lenses. It gets a bit more complicated for mirrors.
09:33
@JohnRennie Ok sir. So the above condition always holds good irrespective of the optical device- lens or mirror or anything else. Am I right, or are there any other exceptions to this rule?
@JohnRennie Yes sir. Just now realised it for concave mirrors even though negative image distance gives a real image and not a virtual as suggested by this.
Is it also applicable in all circumstances for a spherical interface separating two optical media, sir?
Like this:
Medium 1 . . . . . . . . ( . . . . . . . . Medium 2
Yes
moved
09:50
DCP-14-442-17
Two refracting media are separated by a spherical interface as shown in the figure:
$\mu_2$ . . . . . . . . ( . . . . . . . . $\mu_1$
(a) If $\mu_2>\mu_1$, then there cannot be a real image of real object
(b) If $\mu_2>\mu_1$, then there cannot be a real image of virtual object
(c) If $\mu_1>\mu_2$, then there cannot be a virtual image of virtual object
(d) If $\mu_1>\mu_2$, then there cannot be a real image of real object
My approach:
Using the lens maker's formula, I determined the possible signs the image distance $v$ can take for a particular sign of the object distance $u
@JohnRennie: Hi sir. If you're free, could you please reply to the message above? Thank you.
The way I remember how to handle a curved interface is that it's like a plano lens.
So in this case you effectively have a planoconvex lens.
Ok sir. For calculation purposes, I think it's safe to assume a planoconvex lens as a simple biconvex lens. Is this permitted sir?
I'm not sure that makes it any easier ...
As for both planoconvex and bi-convex lens, the focal length for both sides remains the same. We're just neglecting spherical aberration.
Let me draw a quick diagram:
10:03
Ok sir. For virtual object the object distance is positive. And also the image distance is positive as the focal length is positive.
@GuruVishnu OK there's my diagram.
The focal length of the lens is going to be:
@JohnRennie One small issue: I think $R_2=\infty$
$$ \frac{1}{f} = \left(\frac{n_1}{n_2} - 1\right) \frac{1}{R_1} $$
@JohnRennie Yes sir.
@GuruVishnu oops yes.
In (a) $n_2 > n_1$ so $f < 0$ i.e. it is a diverging lens. And for a real object a diverging lens always produces a virtual object. So (a) is true.
10:06
@JohnRennie Yes sir. No problem with (a). The (c) is the one giving me some trouble.
OK. In (c) $n_1 > n_2$ so it is a converging lens.
@JohnRennie Ok sir.
The lens equation is:
$$ \frac{1}{v} = \frac{1}{f} + \frac{1}{u} $$
For both $f$ and $u$ is positive, $v$ is always positive.
Then how can a virtual image be impossible?
It's always the possibility.
For a virtual image $v < 0$ and for a virtual object $u > 0$, and we know $f > 0$.
So let's write our equation with these signs:
$$ \frac{-1}{|v|} = \frac{+1}{|f|} + \frac{+1}{|u|} $$
OK so far?
10:10
@JohnRennie Completely understood my fault. I considered +ve sign for virtual image instead of negative sign. Thank you very much sir :-)
(removed)
 
4 hours later…
14:00
@JohnRennie: Hi sir. Please reply when you find time. Regarding our discussion on Magnetic intensity $\vec H$:

JR0010 : Magnetic intensity

yesterday, 2 hours 38 minutes total – 91 messages, 2 users, 1 star

Bookmarked 2 mins ago by Guru Vishnu

14:12
I don't know why I got confused again sir. Sorry :-(
Intensity of magnetisation is defined as the magnetic moment per unit volume and is independent of the field due to magnetisation. Then how could we eliminate it from the equation: $$\vec H=\frac{\vec B}{\mu_0}-\vec I$$
Thank you.

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