Tactical Movement: Vistaar Mein Jankari

Tactical Movement: Vistaar Mein Jankari 1. Definition (Pari-bhasha) Dushman ke ilake mein ek jagah se doosri jagah tak surakshit pahunchne ke liye, jo dhang aur rules (principles) ek team ya toli apnati hai, use Tactical Movement kehte hain. Iska mukhya uddeshya dushman ki nazaron se bachkar apne mission ko pura karna hota hai. 2. Tactical Movement ke Fayde (Benefits) Command & Control: Commander apni toli par behtar niyantran rakh sakta hai. Suraksha: Dushman ki nazar aur achanak hamle (Ambush) se bacha ja sakta hai. Counter Ambush: Agar dushman hamla kare, to turant palatwar (Pratighat) karne ki kshamta rehti hai. Coordination: Jawano ke beech aapsi talmel (Mutual Support) bana rehta hai. 3. Tactical Movement ke Sidhant (Principles) Yahan aapke dwara bataye gaye points ka sankshipt vivaran hai: Sl. No Point Description 1 Order of Movement Ismein Scout, Section Commander, 2I/C aur baaki jawano ka kram (sequence) tay hota hai. 2 Observation Scout 1 & 2 aage ka 180^\circ area de...

Notes on Wave Optics

🔰Notes on Wave Optics

Magnifying power or magnification of a simple microscope:- M= 1+(D/f)

Magnifying power or magnification of a compound microscope:-

M= L/f0 (1+D/fe)

Here, f0 is the focal length of the objective, fe is the focal length of the eyepiece and L is the length of the microscope tube.

Magnification of astronomical telescope in normal adjustment:-
M = f0/fe

Magnification of astronomical telescope, when the final image is formed at the distance of distinct vision:-
M = (f0/fe) [(fe+D)/D]

Magnifying power M of Galileo’s telescope:-
M = focal length of objective/focal length of eye lens = F/f

Diffraction:- Diffraction is the bending  or spreading of waves that encounter an object ( a barrier or an opening) in their path.

(a) In Fresnel class of diffraction, the source and/or screen are at a finite distance from the aperture.

(b) In Fraunhofer class of diffraction, the source and screen are at infinite distance from the diffracting aperture. Fraunhofer is a special case of Fresnel diffraction.

If Im represents the intensity at O, its value at P is

Iθ = Im (sinα/α)2

Here, α = ?/2 = πa sinθ/λ

A minimum occurs when, sin α = 0 and α is not equal to zero.

so  α = nπ,       n = 1, 2, 3...

So, πa sinθ/λ = nπ

Or, a sinθ = nλ

Angular width of central maxima of diffraction pattern = 2θ1 = 2 sin-1(λ/a)

[ θ1 gives the angular position of first minima]

Polarization: - Polarization of two interfering wave must be same state of polarization or two source of light should be un polarized.

Brewster Law:-
According to this law when un polarized light is incident at polarizing angle (i) on an interface separating a rarer medium from a denser medium, of refractive index m as shown in Fig., below such that,

 µ = tan i

Then light reflected in the rarer medium is completely polarized. Reflected and refractive rays are perpendicular to each other.

Reduction in Intensity:- Intensity of polarized light is 50% of that of the un polarized light, i.e.,
 Ip = Iu/2

Here, Ip = Intensity of polarized light.

Iu = Intensity of un polarized light.

टिप्पणियाँ