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a year ago

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P
Payal Gupta

Contributor-Level 10

12. When tetravalent germanium is doped with trivalent gallium  then some of the positions of the lattice of germanium gets occupied by the gallium. Since the gallium atom has only three valence electrons, the fourth valency of the nearby germanium atom does not get satisfied and hence this place remains vacant. This place is deficient of electrons and is therefore called an electron hole or electron vacancy.

Now, the electron from the neighbouring atom comes and fills the gap and leads to the formation of a hole in its original position. Under the influence of electric fields, the electrons move towards the positively charged plat

...more

New answer posted

a year ago

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V
Vishal Baghel

Contributor-Level 10

The given D.E is

(x+y)dydx=1=x+y=dxdy

=dxdy−x=y Which is of form =dxdy+Px=Q

So,  P= −1&Q=y

∴I.F=e∫Pdy=e∫−1dy=ey

Thus the general solution is of the form,  x* (I.F)=∫Q (I.F)dy+c

New answer posted

a year ago

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V
Vishal Baghel

Contributor-Level 10

The given D.E is

=dydx+y(1+xcotx)x=1 Which is of form dydx+Py=Q

So, P=(1+xcotx)x&Q=1

∫Pdx=∫(1x+xcotxx)dx=log|x|+log|sinx|=log|xsinx|

∴I.F=e∫Pdx−e∫log|xsinx|xsinx

Thus the solution is of the form.

y*xsinx=∫1.xsinxdx+c=x∫sinx−∫ddx∫sinxdxdx+c=−2cosx+∫cosxdx+c=y*xsinx=−xcosx+sinx+c=y=−xcosxsinx+sinxxsinx+cxsinx=y=−cotx+1x+cxsinx

New answer posted

a year ago

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P
Payal Gupta

Contributor-Level 10

11. In semiconductors the gap between conduction band and valence band is small and hence some of the electrons from the valence band can easily jump to the conduction band and shows some conductivity but with rise in the temperature more of the electrons gets jump to the conduction band and thus, their electrical conductivity increases with rise in the temperature.

New answer posted

a year ago

0 Follower 6 Views

V
Vishal Baghel

Contributor-Level 10

The given D.E. is

(1+x)2dy+2xydx=cotxdx=(1+x)2dydx+2xy=cotx

=dydx+2x1+x2*y=cotx1+x2 Which is of form dydx+Py=Q

So , P=2x1+x2&Q=cotx1+x2

∴I.F=e∫Pdx=e∫2x1+x2dx=elog|1+x2|=1+x2

Thus the solution is of the form,

⇒y(1+x2)=∫cotx1+x2*(1+x2)dx+c⇒y(1+x2)=∫cotxdx+c

=log|sinx|+c

⇒y=log|sinx|1+x2+c1+x2=(1+x2)−1log|sinx|+(1+x2)−1c

New answer posted

a year ago

0 Follower 5 Views

A
alok kumar singh

Contributor-Level 10

139. Kindly go through the solution

New answer posted

a year ago

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V
Vishal Baghel

Contributor-Level 10

The given D.E. is

xlogxdydx+y=2xlogx

=dydx+yxlogx=2x2 Which is of form dydx+Py=Q

So, P=1xlogx&Q=2x2

∴I.F=e∫Pdx=e∫1xlogxdx=e∫1xlogxdx=elog|logx|=logx

Thus, the general solution is of the form

y*logx=∫2x2*logxdx+cy.logx=2[logx∫1x2dx−∫ddxlogx∫1x2dx.dx]+c=2[logx*(x−1−1)−∫1x(x−1−1)dx]+c=2[−logxx+∫x−2dx]+c=2[−logxx−(x−1−1)]+c

=ylogx=−2x[logx+1+c]

New answer posted

a year ago

0 Follower 25 Views

P
Payal Gupta

Contributor-Level 10

10. The ZnO crystal becomes yellow oh heating because of the metal excess defect  which is caused due to the presence of extra cations at the interstitial sites and on heating this white crystal it loses oxygen and turns yellow. The reaction involved is given as-

ZnO  Zn2+ + 1 2 O2 + 2e-

Here the excess of Zn2+ ions move to the interstitial sites and electrons to neighbouring interstitial sites.

New answer posted

a year ago

0 Follower 4 Views

V
Vishal Baghel

Contributor-Level 10

The given D.E. is

xdydx+2y=x2logx

⇒dydx+2x.y=xlogx which is of form dydx+Py=Q

So, P=2x&Q=xlogx

∴I.F=e∫Pdx=e∫2xdx=e2logx=elogx2=x2

Thus, the general solution is of the form.

y*x2=∫xlogx.x2dx+c

=∫logxx3dx+c

=logx∫x3dx−∫ddxlogx∫x3dxdx+c=logx.x44−∫14*x44dx+c

=yx2=x44logx−x416+c=y=x24logx−x216+cx2

New answer posted

a year ago

0 Follower 5 Views

A
alok kumar singh

Contributor-Level 10

137. Yes, Let us take f(x)=|x−1|+|x−2|.

So, x = 1, x= 2 divides the real line into three disjoint intervals (−∞,1],[1,2] and [2,∞).

For x∈(−∞,1].

f(x)=−(x−1)+[−(x−2)]=−x+1−x+2=3−2x.

For x∈[1,2]. 

f(x)=(x−1)−(x−2)=1.

For x∈[2,∞)

f(x)=x−1+x−2=2x−3.

Hence, these polynomial fun are all continous and desirable. for all real values of x or, except x = 1 and x = 2.

ie, ∀x∈R−{1,2}.

For differentiavity at x = 1,

LHD = =limx→1−f(x)−f(1)x−1=limx→1−3−2x−1x−1=limx→1−2−2xx−1.

=limx→1−−2(x−1)x−1

=limx→1−−2

= -2

RHD = =limx→1+f(x)−f(1)x−1=limx→1+1−1x−1=limx→1+0x−1=0.

as L.HD ≠ R.HD

f is not differentiable at x =1.

For continuity at x = 1.

L.HL= =limx→1−f(x)=limx→1−=1.

RHL = limx→1+f(x)=limx→1+1=1 \ LHL = RHS

f is continuous at x = 1

For continuity & differentiability at x = 2

=limx→2−f(x)=limx→2−1=1.

  =limx→2+f(x)=limx→2+(2x−3)=4−3=1.

? LHL = RHL

f is continuous at x = 2

=limx→2−f(x)−f(2)x−2=limx→2−1−1x−2=limx→2−=0x−2

  =limx→2+f(x)−f(2)x−2=limx→2+2x−3−1x−2

=limx→2+2(x−2)x−2

=limx→2+2

= 2

? LHD ≠ RHD

f is not differentiable at x = 2.

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