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Post a LessonAnswered on 06/04/2024 Learn CBSE - Class 11/Mathematics/Limits and Derivatives/Unit III: Calculus/Continuity and Differentiability
Sadika
To solve this problem, we will differentiate both sides of the given expression y=(tan−1x)2y=(tan−1x)2 with respect to xx.
Let's denote y=(tan−1x)2y=(tan−1x)2.
First, let's differentiate yy with respect to xx using the chain rule:
dydx=2tan−1x⋅11+x2dxdy=2tan−1x⋅1+x21
Now, let's express dydxdxdy in terms of xx and yy:
dydx=2y⋅11+x2dxdy=2y⋅1+x21
Now, let's differentiate dydxdxdy with respect to xx:
d2ydx2=ddx(2y⋅11+x2)dx2d2y=dxd(2y⋅1+x21)
Using the product rule:
d2ydx2=2⋅11+x2⋅dydx+2y⋅(−2x(1+x2)2)dx2d2y=2⋅1+x21⋅dxdy+2y⋅(−(1+x2)22x)
Substituting dydx=2y⋅11+x2dxdy=2y⋅1+x21:
d2ydx2=2⋅11+x2⋅2y⋅11+x2+2y⋅(−2x(1+x2)2)dx2d2y=2⋅1+x21⋅2y⋅1+x21+2y⋅(−(1+x2)22x)
d2ydx2=4y(1+x2)2−4x2y(1+x2)2dx2d2y=(1+x2)24y−(1+x2)24x2y
d2ydx2=4y−4x2y(1+x2)2dx2d2y=(1+x2)24y−4x2y
d2ydx2=4(y−x2y)(1+x2)2dx2d2y=(1+x2)24(y−x2y)
Now, let's substitute y=(tan−1x)2y=(tan−1x)2 back into the expression:
d2ydx2=4((tan−1x)2−x2(tan−1x)2)(1+x2)2dx2d2y=(1+x2)24((tan−1x)2−x2(tan−1x)2)
d2ydx2=4(tan−1x)2(1−x2)(1+x2)2dx2d2y=(1+x2)24(tan−1x)2(1−x2)
Now, let's manipulate the expression d2ydx2dx2d2y to match the left side of the given expression (x2+1)2y2+2x(x2+1)y′=2(x2+1)2y2+2x(x2+1)y′=2:
(x2+1)2y2+2x(x2+1)y′=(x2+1)2((tan−1x)2)2+2x(x2+1)dydx(x2+1)2y2+2x(x2+1)y′=(x2+1)2((tan−1x)2)2+2x(x2+1)dxdy
(x2+1)2y2+2x(x2+1)y′=(x2+1)2(tan−1x)4+2x(x2+1)⋅2y1+x2(x2+1)2y2+2x(x2+1)y′=(x2+1)2(tan−1x)4+2x(x2+1)⋅1+x22y
(x2+1)2y2+2x(x2+1)y′=4(x2+1)2(tan−1x)2(1+x2)2+4x(x2+1)y1+x2(x2+1)2y2+2x(x2+1)y′=(1+x2)24(x2+1)2(tan−1x)2+1+x24x(x2+1)y
Now, let's simplify this expression:
(x2+1)2y2+2x(x2+1)y′=4(x2+1)2(tan−1x)2+4x(x2+1)(tan−1x)2(1+x2)(1+x2)2(x2+1)2y2+2x(x2+1)y′=(1+x2)24(x2+1)2(tan−1x)2+4x(x2+1)(tan−1x)2(1+x2)
(x2+1)2y2+2x(x2+1)y′=4(x2+1)2(tan−1x)2+4x(x2+1)(tan−1x)2(1+x2)(1+x2)2(x2+1)2y2+2x(x2+1)y′=(1+x2)24(x2+1)2(tan−1x)2+4x(x2+1)(tan−1x)2(1+x2)
(x2+1)2y2+2x(x2+1)y′=4(x2+1)2(tan−1x)2+4x(x2+1)2(tan−1x)2(1+x2)2(x2+1)2y2+2x(x2+1)y′=(1+x2)24(x2+1)2(tan−1x)2+4x(x2+1)2(tan−1x)2
(x2+1)2y2+2x(x2+1)y′=4(x2+1)2(tan−1x)2(1+x2+x)(1+x2)2(x2+1)2y2+2x(x2+1)y′=(1+x2)24(x2+1)2(tan−1x)2(1+x2+x)
(x2+1)2y2+2x(x2+1)y′=4(x2+1)2(tan−1x)2(x2+1)(1+x2)2(x2+1)2y2+2x(x2+1)y′=(1+x2)24(x2+1)2(tan−1x)2(x2+1)
(x2+1)2y2+2x(x2+1)y′=4(x2+1)(tan−1x)2(x2+1)2y2+2x(x2+1)y′=4(x2+1)(tan−1x)2
(x2+1)2y2+2x(x2+1)y′=4(x2+1)y2(x2+1)2y2+2x(x2+1)y′=4(x2+1)y2
Thus, we have verified that (x2+1)2y2+2x(x2+1)y′=2(x2+1)2y2+2x(x2+1)y′=2.
Answered on 06/04/2024 Learn CBSE - Class 11/Mathematics/Limits and Derivatives/Unit III: Calculus/Continuity and Differentiability
Sadika
To verify Rolle's Theorem for the function y=x2+2y=x2+2 on the interval [−2,2][−2,2], we need to check three conditions:
Let's check each condition:
Continuity: The function y=x2+2y=x2+2 is a polynomial function and is continuous everywhere. Therefore, it is continuous on the closed interval [−2,2][−2,2].
Differentiability: The function y=x2+2y=x2+2 is a polynomial function and is differentiable everywhere. Therefore, it is differentiable on the open interval (−2,2)(−2,2).
Endpoints: y(−2)=(−2)2+2=4+2=6y(−2)=(−2)2+2=4+2=6 y(2)=(2)2+2=4+2=6y(2)=(2)2+2=4+2=6
So, y(−2)=y(2)y(−2)=y(2).
Since all three conditions of Rolle's Theorem are satisfied, there exists at least one cc in the open interval (−2,2)(−2,2) such that f′(c)=0f′(c)=0, where f(x)=x2+2f(x)=x2+2.
Now, let's find the derivative of y=x2+2y=x2+2:
y′=ddx(x2+2)=2xy′=dxd(x2+2)=2x
To find the critical point(s), we set y′=0y′=0: 2x=02x=0 x=0x=0
So, f′(0)=0f′(0)=0.
Thus, Rolle's Theorem is verified for the function y=x2+2y=x2+2 on the interval [−2,2][−2,2], and there exists at least one point cc in the open interval (−2,2)(−2,2) where the derivative f′(c)f′(c) is equal to zero.
Answered on 06/04/2024 Learn CBSE - Class 11/Mathematics/Limits and Derivatives/Unit III: Calculus/Continuity and Differentiability
Sadika
To differentiate sin(2x)sin(2x) with respect to ecos(x)ecos(x), we can use the chain rule. Let u=ecos(x)u=ecos(x), then dudx=−esin(x)dxdu=−esin(x).
Now, we have:
ddu(sin(2x))=ddu(sin(2x))×dudxdud(sin(2x))=dud(sin(2x))×dxdu
Using the chain rule:
ddu(sin(2x))=dd(2x)(sin(2x))×d(2x)dxdud(sin(2x))=d(2x)d(sin(2x))×dxd(2x)
=cos(2x)×2=cos(2x)×2
=2cos(2x)=2cos(2x)
Now, we need to multiply this by dudxdxdu:
=2cos(2x)×(−esin(x))=2cos(2x)×(−esin(x))
=−2ecos(2x)sin(x)=−2ecos(2x)sin(x)
So, the derivative of sin(2x)sin(2x) with respect to ecos(x)ecos(x) is −2ecos(2x)sin(x)−2ecos(2x)sin(x).
Answered on 06/04/2024 Learn CBSE - Class 11/Mathematics/Limits and Derivatives/Unit III: Calculus/Continuity and Differentiability
Sadika
To differentiate the equation xy=ex−yxy=ex−y implicitly with respect to xx, we will use the product rule and the chain rule.
Given the equation:
xy=ex−yxy=ex−y
Taking the natural logarithm (ln) of both sides:
ln(xy)=ln(ex−y)ln(xy)=ln(ex−y)
ln(xy)=x−yln(xy)=x−y
Now, differentiating both sides with respect to xx:
ddx(ln(xy))=ddx(x−y)dxd(ln(xy))=dxd(x−y)
Using the chain rule and the product rule on the left side:
1xy(xdydx+y)=1xy1(xdxdy+y)=1
Now, solve for dydxdxdy:
xdydx+y=xyxdxdy+y=xy
xdydx=xy−yxdxdy=xy−y
dydx=xy−yxdxdy=xxy−y
dydx=y(x−1)xdxdy=xy(x−1)
So, the derivative of yy with respect to xx is given by:
dydx=y(x−1)xdxdy=xy(x−1)
Answered on 06/04/2024 Learn CBSE - Class 11/Mathematics/Limits and Derivatives/Unit III: Calculus/Continuity and Differentiability
Sadika
To show that x2y2+xyy′+y=0x2y2+xyy′+y=0 for y=3cos(logx)+4sin(logx)y=3cos(logx)+4sin(logx), we'll first find y′y′, the derivative of yy with respect to xx, and then substitute yy and y′y′ into the expression x2y2+xyy′+yx2y2+xyy′+y.
Given: y=3cos(logx)+4sin(logx)y=3cos(logx)+4sin(logx)
We'll find y′y′, the derivative of yy with respect to xx, using the chain rule:
dydx=ddx[3cos(logx)+4sin(logx)]dxdy=dxd[3cos(logx)+4sin(logx)]
Using the chain rule:
dydx=−3sin(logx)⋅1x+4cos(logx)⋅1xdxdy=−3sin(logx)⋅x1+4cos(logx)⋅x1
dydx=−3sin(logx)+4cos(logx)xdxdy=x−3sin(logx)+4cos(logx)
Now, we'll substitute yy and y′y′ into the expression x2y2+xyy′+yx2y2+xyy′+y:
x2y2+xyy′+yx2y2+xyy′+y
=x2(3cos(logx)+4sin(logx))2+x(3cos(logx)+4sin(logx))(−3sin(logx)+4cos(logx)x)+(3cos(logx)+4sin(logx))=x2(3cos(logx)+4sin(logx))2+x(3cos(logx)+4sin(logx))(x−3sin(logx)+4cos(logx))+(3cos(logx)+4sin(logx))
Now, we'll simplify this expression.
Let's denote u=cos(logx)u=cos(logx) and v=sin(logx)v=sin(logx). Then u2+v2=1u2+v2=1 (due to the Pythagorean identity).
=x2(3u+4v)2+x(3u+4v)(−3v+4ux)+(3u+4v)=x2(3u+4v)2+x(3u+4v)(x−3v+4u)+(3u+4v)
=x2(9u2+24uv+16v2)+x(−9uv+12u+12v2x)+3u+4v=x2(9u2+24uv+16v2)+x(x−9uv+12u+12v2)+3u+4v
=9x2u2+24x2uv+16x2v2−9uv+12u+12v2+3u+4v=9x2u2+24x2uv+16x2v2−9uv+12u+12v2+3u+4v
=9x2u2+24x2uv+16x2v2−9uv+3u+12u+12v2+4v=9x2u2+24x2uv+16x2v2−9uv+3u+12u+12v2+4v
=9x2u2+24x2uv+16x2v2−9uv+15u+12v2+4v=9x2u2+24x2uv+16x2v2−9uv+15u+12v2+4v
Now, using the Pythagorean identity u2+v2=1u2+v2=1:
=9x2+24x2+16x2−9uv+15u+12v2+4v=9x2+24x2+16x2−9uv+15u+12v2+4v
=(9+24+16)x2−9uv+15u+12v2+4v=(9+24+16)x2−9uv+15u+12v2+4v
=49x2−9uv+15u+12v2+4v=49x2−9uv+15u+12v2+4v
Now, substitute uu and vv:
=49x2−9sin(logx)cos(logx)+15cos(logx)+12sin2(logx)+4sin(logx)=49x2−9sin(logx)cos(logx)+15cos(logx)+12sin2(logx)+4sin(logx)
=49x2−9sin(2logx)+15cos(logx)+12sin2(logx)+4sin(logx)=49x2−9sin(2logx)+15cos(logx)+12sin2(logx)+4sin(logx)
=49x2−9sin(2logx)+15cos(logx)+12(1−cos2(logx))+4sin(logx)
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