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New answer posted

a year ago

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V
Vishal Baghel

Contributor-Level 10

⇒dydx=x3−3xy2y3−3x2y..........(1)

This is a homogenous equation. To simplify it, we need to make the substitution as:

y=vx⇒ddx(y)=ddx(vx)⇒dydx=v+xdvdx

Substituting the values of y and dvdx in equation (1), we get:

v+xdvdx=x3−3x(vx)2(vx)3−3x2(vx)⇒v+xdvdx=1−3v2v3−3v⇒xdvdx=1−3v2v3−3v−v⇒xdvdx=1−3v2−v(v3−3v)v3−3v⇒xdvdx=1−v4v3−3v⇒(v3−3v1−v4)dv=dxx

Integrating both sides, we get:

∫(v3−3v1−v4)dv=logx+logC'.........(2)Now,∫(v3−3v1−v4)dv=∫v3dv1−v4−3∫vdv1−v4⇒∫(v3−3v1−v4)dv=I1−3I2,Where,I1=∫v3dv1−v4andI2=∫vdv1−v4...........(3)

Let,1−v4=t.∴ddv(1−v4)=dtdv⇒−4v3=dtdv⇒v3dv=−dt4Now,I1=∫−dt4=−logt=−14log(1−v4)

And,I2=∫vdv1−v4=∫vdv1−(v2)2Let,v2=p.∴ddv(v2)=dpdv⇒2v=dpdv⇒vdv=p2⇒I2=12∫dp1−p2=12*2log|1+p1−p|=14log|1+v21−v2|

Substituting the values of I1 and I2 in equation (3), we get:

∫(v3−3v1−v4)dv=−14log(1−v4)−34log|1+v21−v2|

Therefore, equation (2) becomes:

14log(1−v4)−34log|1+v21−v2|=logx+logC'⇒−14log[(1−v4)(1+v21−v2)]=logC'x⇒(1+v2)4(1−v2)2=(C'x)−4⇒(1+y2x2)4(1−y2x2)2=1C'4x4⇒(x2+y2)4x4(x2−y2)2=1C'4x4⇒(x2−y2)2=C'4(x2+y2)4⇒(x2−y2)=C'2(x2+y2)2⇒x2−y2=C(x2+y2)2,whereC=C'2

Hence, the given result is proved.

New answer posted

a year ago

0 Follower 7 Views

V
Vishal Baghel

Contributor-Level 10

Equation of the given family of curves is  (x−a)2+2y2=a2

(x−a)2+2y2=a2⇒x2+a2−2ax+2y2=a2⇒2y2=2ax−x2..........(1)

Differentiating with respect to x, we get:

2ydydx=2a−2x2⇒dydx=a−x2y⇒dydx=2a−2x24xy..........(2)

From equation (*1), we get:

2ax=2y2+x2

On substituting this value in equation (3), we get:

dydx=2y2+x2−2x24xy⇒dydx=2y2−x24xy

Hence, the differential equation of the family of curves is given as dydx=2y2−x24xy

New answer posted

a year ago

0 Follower 5 Views

P
Payal Gupta

Contributor-Level 10

19. Option (i) Same in all directions is correct since quartz glass is an amorphous solid showing isotropic properties and hence exhibits the same values of refractive index when measured along different directions.

New answer posted

a year ago

0 Follower 17 Views

V
Vishal Baghel

Contributor-Level 10

(i) yae2+be−x+x2

Differentiating both sides with respect to x, we get:

dydx=addx(ex)+bddx(e−x)+ddx(x2)⇒dydx=aex−be−x+2x

Again, differentiating both sides with respect to x, we get:

d2ydx2=aex−be−x+2x

Now, on substituting the values of dydx and d2ydx2 in the differential equation, we get:

L.H.S

xd2ydx2+2dydx−xy+x2−2=x(aex−be−x+2)+2(aex−be−x+2x)−x(aex+be−x+x2)+x2−2=(xaex−bxe−x+2x)+(2aex−2be−x+4x)−(axex+bxe−x+x3)+x2−2=2aex−2be−x+x2+6x−2≠0

Therefore, Function given by equation (i) is a solution of differential equation. (ii).

(ii) y=ex(acosx+bsinx)=aexcosx+bexsinx

Differentiating both sides with respect to x, we get:

dydx=a.ddx(excosx)+b.ddx(exsinx)⇒dydx=a(excosx−exsinx)+b.(exsinx+excosx)⇒dydx=(a+b)excosx+(b−a)exsinx

Again, differentiating both sides with respect to x, we get:

d2ydx2=(a+b).ddx(excosx)(b−a)ddx(exsinx)⇒d2ydx2=(a+b).[excosx−exsinx]+(b−a)[exsinx+excosx]⇒d2ydx2=ex[(a+b)(cosx−sinx)+(b−a)(sinx+cosx)]⇒d2ydx2=ex[acosx−asinx+bcosx−bsinx+bsinx+bcosx−asinx−acosx]⇒d2ydx2=[2ex(bcosx−asinx)]

Now, on substituting the values of d2ydx2 and dydx in the L.H.S of the given differential equation, we get:

d2ydx2+2dydx+2y=2ex(bcosx−asinx)−2ex[(a+b)cosx+(b−a)sinx]+2ex(acosx+bsinx)=ex[(2bcosx−2asinx)−(2acosx+2bcosx)−(2bsinx−2asinx)+(2acosx+2bsinx)]=ex[(2b−2a−2b+2a)cosx]+ex[(−2a−2b+2a+2b)sinx]=0

Therefore, Function given by equation (i) is solution of differential equation (ii)

(iii)&nb

...more

New answer posted

a year ago

0 Follower 8 Views

P
Payal Gupta

Contributor-Level 10

18. Option (iv) is correct since in antiferromagnetic substances the domains  are oppositely oriented and hence they cancel out each other's magnetic moments. 

New answer posted

a year ago

0 Follower 10 Views

P
Payal Gupta

Contributor-Level 10

17. Option (ii) Quartz glass (SiO2) is correct since quartz glass (SiO2)is amorphous in nature as there is no long range ordered arrangement of the constituent particles being present in it and hence it is an amorphous solid.

New answer posted

a year ago

0 Follower 4 Views

V
Vishal Baghel

Contributor-Level 10

(i) Given: Differential equation   d2ydx2+5x(dydx)2−6y=logx

The highest order derivative present in this differential equation is d2ydx2 and hence order of this differential equation if 2.

The given differential equation is a polynomial equation in derivatives and highest power of the highest order derivative d2ydx2 is 1.

Therefore, Order = 2, Degree = 1

(ii) Given: Differential equation (dydx)3−4(dydx)2+7y=sinx

The highest order derivative present in this differential equation is dydx and hence order of this differential equation if 1.

The given differential equation is a polynomial equation in derivatives and highest power of the highest order derivativ

...more

New answer posted

a year ago

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P
Payal Gupta

Contributor-Level 10

16. Option (ii) Isotropic nature is correct since crystalline solids exhibit anisotropic properties like refractive index, electrical resistance etc. Since these are found to have different values when measured along different directions in the same crystal and hence they are not isotropic in nature. 

New answer posted

a year ago

0 Follower 4 Views

V
Vishal Baghel

Contributor-Level 10

The given D.E. is

(1−y2)dxdy+yx=∝y(−1<y<1)

dxdy+y1−y2*x=∝y1−y2 which is of form

dxdy+Px=Q&P=y1−y2&Q=∝y1−y2∫pdx=∫y1−y2dx=−12∫−2y1−y2dx

=−12log|1−y2|=log[1−y2]−12

∴I.F=e∫Pdx=elog[1−y2]−12=[1−y2]−12

∴ option (D ) is correct.

New answer posted

a year ago

0 Follower 3 Views

P
Payal Gupta

Contributor-Level 10

15. Option (ii) Low temperature is correct since at sufficiently low temperature, the thermal energy is low, so the intermolecular forces bring the molecules of a substance closer so that they cling to one another and occupy fixed positions. They keep on vibrating about their fixed positions. Such conditions favours the existence of the substance in solid state. 

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