Physics Ncert Solutions Class 12th

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New answer posted

4 months ago

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Payal Gupta

Contributor-Level 10

This is a long answer type question as classified in NCERT Exemplar

applying ohm's law

I=E/R=d / R d t

I= dQ/dt or dQ/dt= d / R d t

Q (t1)-Q (t2)= 1 R [ t1- t2]

t1= L1 μ 0 2 π x L 2 + x d x x I t1

= μ 0 L 1 2 π I1in [ L 2 + x x ]

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Payal Gupta

Contributor-Level 10

This is a long answer type question as classified in NCERT Exemplar

B= ? 0 I 2 R (ouside the paper)

Flux= ? 0 I 2 R l ? x 0 x d r r = ? 0 I 2 R in x x 0

Induced emf= e/R=I

Induced current = 1 R d ? d t = e R = ? 0 I ? 2 ? R in x x 0

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Payal Gupta

Contributor-Level 10

This is a long answer type question as classified in NCERT Exemplar

At t=o t=T/8= π / 4 w  the rod will make contact with side BD.at any time 0 π / 4 w

So magnetic flux through area ODQ is = B * a r e a O Q D = B * 1 2 Q D * O D

=B * 1 l t a n θ 2 * l

= 1 2 B L 2 w t a n θ = 1 2 B L 2 w s e c 2 w t

I=e/R

And R= λ x = λ l c o s w t  so I= 1 2 B L w c o s w t λ

Same result for other side too

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Payal Gupta

Contributor-Level 10

This is a long answer type question as classified in NCERT Exemplar

Let us assume that the parallel wires at are y= 0, i.e., along x-axis and y= l. At t= 0, XY has x = 0 i.e., along y-axis.

(i) Let the wire be at x x = (t) at time t.

The magnetic flux linked with the loop is given by

φ = B.A= Bacos0= BA

magnetic flux = B(t)(lx(t))

total emf = emf due to change in field along XYAC+ the motional emf across XY

E= - d d t  = - d B ( t ) d t lx(t)- B(t)lv(t)

Electric current in clockwise direction is I= E/r

So force is F= ilBsin90=ilB

Force = I B ( t ) R [- d B t d t I x t - B ( t ) I v ( t ) ]i

Applying newton 2nd law

m d 2 x d t 2 = I 2 B t d B R d t x ( t ) - I 2 B 2 t d x R d t

(ii) d B d t =0

Substituting in eqn 1

d 2 x d t 2 + I 2 B 2 t d x m R d t =0

d v d t + I 2 B 2 v m R =o

V= Aexp ( I 2 B 2 v m R )=0

(iii) p= I2R= I 2 B 2 v 2 R R 2 = B 2 I 2 R u 0 2 exp(-2

...more

New answer posted

4 months ago

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Payal Gupta

Contributor-Level 10

This is a long answer type question as classified in NCERT Exemplar

Let us assume that parallel wires at are y=0 i.e along x-axis and y=d.at t=0, AB has x=0 i.e along y-axis and moves with a velocity v

Motional emf across AB is = (B0sinwt)vd (-j)

Emf due to change in field along OBAC = -B0wcoswt x (t)d

Total emf in the circuit = emf due to change in field (along OBAC)+ the motional emf across AB= - B0d {wx coswt+v sinwt}

Electric current in clockwise direction is given by =   B 0 d R   (wxcoswt+vsinwt)

The force acting on the conductor is given by F= iLbsin90=iLb

Substituting the values

F=   B 0 d R   (wx coswt+v sinwt) * d * B0si

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4 months ago

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Payal Gupta

Contributor-Level 10

This is a multiple choice answer as classified in NCERT Exemplar

(c), (d) Case A: When key K is kept closed and plates of capacitors are moved apart using insulating handle.
The battery maintains the potential difference across connected capacitor in every circumstance. The separation between two plates increases which in turn decreases its capacitance (C=? 0A/d)and potential difference across connected capacitor continue to be the same as capacitor is still connected with battery. So the charge stored decreases as Q = CV.

Case B: When key K is opened and plates of capacitors are moved apart using insulating handle.The charge s

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4 months ago

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Payal Gupta

Contributor-Level 10

This is a multiple choice answer as classified in NCERT Exemplar

(a, b) The potential of a body is due to charge of the body and due to the charge of surrounding. If there are no charges anywhere else outside, then the potential of the body will be due to its own charge. If there is a cavity inside a conducting body, then charge can be placed inside the body. Hence there must be charges on its surface or inside itself.  Also The charge resides on the outer surface of a closed charged conductor. Hence there cannot be any charge in the body of the conductor.

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4 months ago

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Payal Gupta

Contributor-Level 10

This is a multiple choice answer as classified in NCERT Exemplar

(a), (d) Initially key K1 is closed and key K2 is open, the capacitor C1 is charged by battery and capacitor C2 is still uncharged. Now K1 is opened and K2 is closed, the capacitors C1 and C2 both are connected in parallel. The charge stored by capacitor C1, gets redistributed between C1 and C2 till their potentials become same, i.e., V2 = V1.
By law of conservation of charge, the charge stored in capacitor Cx is equal to sum of charges on capacitors C1 and C2 when K1 is opened and K2 is closed, i.e.,  Q

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New question posted

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New answer posted

4 months ago

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P
Payal Gupta

Contributor-Level 10

This is a multiple choice answer as classified in NCERT Exemplar

(b), (c) We know, the electric field intensity E and electric potential V are dV related as E =- dV/dr or we can write |E|=ΔV/Δr

The electric field intensity E and electric potential V are related as E = 0 and for V = constant, dV/dr=0 this imply that electric field intensity E = 0.

If some charge is present inside the region then electric field cannot be zero at that region, for this V = constant is not valid.

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