Monday, August 26, 2024

Local non-intrinsic property of surface

MEAN
TT

Tuesday, August 13, 2024

Weingarten equations

MEAN






Weingarten equations

Weingarten equations is about derivative of the unit normal vector \( \vec{N} \).
These equations were established in 1861 by German mathematician Julius Weingarten.
The Weingarten equation is
\( {H^2}\vec{N}_1=( FM-GL )\vec{r}_1+( FL-EM )\vec{r}_2\) and
\( {H^2}\vec{N}_2=( FN-GM )\vec{r}_1+( FM-EN )\vec{r}_2\)
The matrix equivalent of the Weingarten equation is
\( {H^2} \begin{pmatrix} \vec{N}_1 \\ \vec{N}_2 \end{pmatrix}=\begin{pmatrix} FM-GL & FL-EM \\ FN-GM & FM-EN \end{pmatrix} \begin{pmatrix} \vec{r}_1 \\ \vec{r}_2 \end{pmatrix} \)


In a surface, show that

  1. \( {H^2}\vec{N}_1=( FM-GL )\vec{r}_1+( FL-EM )\vec{r}_2\) and
  2. \( {H^2}\vec{N}_2=( FN-GM )\vec{r}_1+( FM-EN )\vec{r}_2\)

Also, verify that
\( H\vec{N}_1\times \vec{N}_2=( LN-{M^2} )\vec{N}\)
Proof
Let \( S:\vec{r}=\vec{r}( u,v )\) be a surface and \( \vec{N}\) be unit normal.
Then,
\( d\vec{N}\) lies in tangent plane of S. Thus, we write
\( \vec{N}_1=a\vec{r}_1+b\vec{r}_2\) (A)
\( \vec{N}_2=c\vec{r}_1+d\vec{r}_2\) (B)
Taking dot product on both sides of (A) by \( \vec{r}_1\) we get
\( \vec{N}_1.\vec{r}_1=a\vec{r}_1^2+b\vec{r}_1.\vec{r}_2\)
or \( -L = aE+bF \)
or \( aE+b F + L =0 \) (1)
Again,
Taking dot product on both sides of (A) by \( \vec{r}_2\) we get
\( \vec{N}_1.\vec{r}_2=a\vec{r}_1.\vec{r}_2+b\vec{r}_2^2\)
or \( -M = a F +b G \)
or \( aF+bG+M=0 \) (2)
Now,
The cross-multiplication method is applied.
Solving, equations (1) and (2), for \( a \) and \( b \) ,we get
\( \frac{a}{ FM-GL } = \frac{b}{ FL-EM }= \frac{1}{EG-F^2}\)
or \( \frac{a}{ FM-GL } = \frac{b}{ FL-EM }= \frac{1}{H^2}\)
Equating first and third identity, similarly equating second and third identity, we get
or \( a=\frac{ FM-GL }{ H^2} , b= \frac{ FL-EM }{ H^2}\)
Substituting, value of \( a \) and \( b\) in (A) we get
\( \vec{N}_1=a\vec{r}_1+b\vec{r}_2\)
or \( \vec{N}_1=\frac{ FM-GL }{ H^2} \vec{r}_1+\frac{ FL-EM }{ H^2} \vec{r}_2\)
or \( {H^2}\vec{N}_1=( FM-GL )\vec{r}_1+( FL-EM )\vec{r}_2\)
The first Weingarten equation established.

Similarly,
Taking dot product on both sides of (B) by \( \vec{r}_1\) we get
\( \vec{N}_2.\vec{r}_1=c\vec{r}_1^2+d\vec{r}_1.\vec{r}_2\)
or \( -M = cE+dF \)
or \( cE+d F + M =0 \) (3)
Again,
Taking dot product on both sides of (B) by \( \vec{r}_2\) we get
\( \vec{N}_2.\vec{r}_2=c\vec{r}_1.\vec{r}_2+d\vec{r}_2^2\)
or \( -N = c F +d G \)
or \( cF+dG+N=0 \) (4)
Now,
Solving, equations (3) and (4), for \( c \) and \( d \) ,we get
The cross-multiplication method is applied.
\( \frac{c}{ FN-GM } = \frac{d}{ FM-EN }= \frac{1}{EG-F^2}\)
or \( \frac{c}{ FN-GM } = \frac{d}{ FM-EN }= \frac{1}{H^2}\)
Equating first and third identity, similarly equating second and third identity, we get
\( c=\frac{ FN-GM }{ H^2} , d= \frac{ FM-EN }{ H^2}\)
Substituting, value of \( c \) and \(d\) in (B) we get
\( \vec{N}_2=c\vec{r}_1+d\vec{r}_2\)
or \( \vec{N}_2=\frac{ FN-GM }{ H^2} \vec{r}_1+\frac{ FM-EN }{ H^2} \vec{r}_2\)
or \( H^2 \vec{N}_2=( FN-GM ) \vec{r}_1+( FM-EN ) \vec{r}_2\)
The second Weingarten equation established.

Finally,
The Weingarten equation is
\( {H^2}\vec{N}_1=( FM-GL )\vec{r}_1+( FL-EM )\vec{r}_2\) and
\( {H^2}\vec{N}_2=( FN-GM )\vec{r}_1+( FM-EN )\vec{r}_2\)
Taking cross product of Weingarten equations, we get
\( {H^2}\vec{N}_1 \times {H^2}\vec{N}_2 = \left\{ ( FM-GL )\vec{r}_1 + ( FL-EM )\vec{r}_2 \right \} \times \left \{ ( FN-GM )\vec{r}_1 + ( FM-EN )\vec{r}_2 \right \} \)
or\( H^4\vec{N}_1 \times \vec{N}_2 = ( FM-GL )\vec{r}_1 \times ( FM-EN ) \vec{r}_2 + (FL-EM )\vec{r}_2 \times ( FN-GM )\vec{r}_1 \)
or\( H^4\vec{N}_1 \times \vec{N}_2 = ( FM-GL ) ( FM-EN ) (\vec{r}_1 \times \vec{r}_2 )+ (FL-EM ) ( FN-GM ) ( \vec{r}_2 \times \vec{r}_1) \)
or\( H^4\vec{N}_1 \times \vec{N}_2 = ( FM-GL ) ( FM-EN ) ( \vec{r}_1 \times \vec{r}_2 ) - (FL-EM ) ( FN-GM ) (\vec{r}_1 \times \vec{r}_2) \)
or\( H^4\vec{N}_1 \times \vec{N}_2 = ( FM-GL ) ( FM-EN ) H \vec{N} - (FL-EM ) ( FN-GM ) H \vec{N} \)
or\( H^4 \vec{N}_1 \times \vec{N}_2 = \{ ( FM-GL ) ( FM-EN ) - (FL-EM ) ( FN-GM ) \} H\vec{N} \)
or\( {H^4}\vec{N}_1 \times \vec{N}_2 = ( EG-F^2 ) ( LN-M^2 ) H \vec{N} \)
or\( {H^4}\vec{N}_1 \times \vec{N}_2 = H^2 ( LN-M^2 ) H \vec{N} \)
or\( {H^4}\vec{N}_1 \times \vec{N}_2 = H^3 ( LN-M^2 ) \vec{N} \)
or\( H\vec{N}_1 \times \vec{N}_2 = ( LN-M^2 ) \vec{N} \)
This completes.

Prove that, a oint \( p \) on a Surface is Umbilical if and only if \( \mu^2 = K \)
We know that
A point \( p \) on a surface is called umbilical if and only if the principal curvatures at \( p \) are equal, i.e., \( k_1 = k_2 \). So, If \( p \) is umbilical, then \(\mu = \frac{k_1 + k_2}{2} = \frac{k + k}{2} = k\)
Next
\(K = k_1 k_2 = k \times k = k^2\)
This shows that if \( p \) is an umbilical point, then \( \mu^2 = K \)


Double family of curves

MEAN






Double family of curves

Let S: \(\vec{r}=\vec{r}(u,v) \) be a surface then the quadratic differential equation
\( Pdu^2+2Qdudv+Rdv^2=0\)
or\( P \left( \frac{du}{dv}\right)^2+2Q\left( \frac{du}{dv}\right)+R=0 \)
where P,Q,R are continuous function of u,v and do not vanish together, is called double family of curves on the surface.

Condition for orthogonality of double family

Let S: \(\vec{r}=\vec{r}(u,v) \) be a surface, and
\( Pdu^2+2Qdudv+Rdv^2=0\)
or\( P \left( \frac{du}{dv}\right)+2Q\left( \frac{du}{dv}\right)+R=0 \)
be double family of curves.
If \(\left( \frac{\lambda}{\mu}, \frac{\lambda '}{\mu '}\right) \) be the roots of the curves, then.
\( \frac{\lambda}{\mu}+ \frac{\lambda '}{\mu '}= \frac{-2Q}{P}\) and \( \frac{\lambda}{\mu}. \frac{\lambda '}{\mu '}= \frac{R}{P}\)
Now, the curves are orthogonal if
\( E \frac{\lambda}{\mu}. \frac{\lambda '}{\mu '}+ F\left( \frac{\lambda}{\mu}+\frac{\lambda '}{\mu '}\right)+G=0\)
or\( E \left ( \frac{R}{P} \right ) + F \left (\frac{-2Q}{P} \right )+G=0\)
or\( ER-2QF+GP=0\)




Theorem 1

The necessary and sufficient condition for parametric curves to be orthogonal is F=0
Proof
Let \(S: \vec{r}=\vec{r}(u,v)\) be a surface with parametric curves u =constant and v =constant on it.
Then, differential equation of parametric curves is
dudv=0 (i)
Also, differential equation of double family of curves is
\(P{du}^2+2Qdudv+R{dv}^2=0\) (ii)
Comparing (i) and (ii) we get
P=0, Q≠0 and R=0
Now, necessary and sufficient condition for parametric curves to be orthogonal is
ER-2QF+GP=0
or E.0-2QF+G.0=0
or F=0

Theorem 2

Show that parametric curves form an orthogonal system on a sphere x=asinu cosv,y=asinu sinv,z=acosu.
Solution
The sphere is
x=asinucosv,y=asinusinv,z=acosu
or \( \vec{r}=(a \sin u \cos v, a \sin u \sin v,a \cos u \) (i)
By successive differentiation w. r. to. u and v, we get
\( \vec{r}_1=(a \cos u \cos v,a \cos u \sin v,-a \sin u \)
\( \vec{r}_2=(-a \sin u \sin v,a \sin u \cos v,0 \)
Now, the fundamental coefficient are
\( F=\vec{r}_1.\vec{r}_2=0\)
Hence, the parametric curves on a sphere form an orthogonal system.

Theorem 3

Prove that, if θ is angle between two directions of \(Pdu^2+2Qdudv+Rdv^2=0\) then \( \tan \theta =\frac{2H \sqrt{Q^2-PR}}{ER-2FQ+GP} \)
Solution
The double family of curves is
\(Pdu^2+2Qdudv+Rdv^2=0\)
or \(P \left ( \frac{du}{dv} \right )^2+2Q \frac{du}{dv}+R=0\)
Let \( \left ( \frac{l}{m} ,\frac{l'}{m'} \right ) \) be the roots, then
\( \frac{l}{m}+\frac{l'}{m'}=\frac{-2Q}{P}\) and \( \frac{l}{m}.\frac{l'}{m'}=\frac{R}{P}\)
Hence
\( \cos \theta =Ell'+F(lm'+l'm)+Gmm'\)
or \( \cos \theta =E \left( \frac{l}{m}.\frac{l'}{m'}\right )+F \left( \frac{l}{m}+\frac{l'}{m'}\right )+G\)
or \( \cos \theta =E \left( \frac{R}{P} \right ) +F \left( \frac{-2Q}{P} \right )+G\)
or \( \cos \theta =\frac{ER-2FQ+GP}{P} \) (A)
Again
\( \sin \theta =H(lm'-l'm)\)
or \( \sin \theta =H\left( \frac{l}{m}-\frac{l'}{m'}\right )\)
or \( \sin \theta =H \sqrt{\left( \frac{l}{m}+\frac{l'}{m'}\right )^2-4 \left( \frac{l}{m}.\frac{l'}{m'}\right ) } \)
or \( \sin \theta =H \sqrt{\left( \frac{-2Q}{P} \right )^2-4 \left( \frac{R}{P} \right ) } \)
or \( \sin \theta =\frac{2H \sqrt{Q^2-PR}}{P} \) (B)
Thus, using (A) and (B), we get
\( \tan \theta =\frac{2H \sqrt{Q^2-PR}}{ER-2FQ+GP} \)
This completes the solution

Orthogonal trajectories

MEAN






Orthogonal trajectories

Let S: \(\vec{r}=\vec{r}(u,v) \) be a surface with family of curves
\( \phi(u,v)=c\) (i)
\( \psi(u,v)=c_1\) (ii)
Now, family (i) and (ii) are called orthogonal trajectories, if the curves of the both families are orthogonal at each of their intersection.

Examples

As we know, family of curves \( xy=c;c\neq 0 \) and \( x^2-y^2=c;c\neq 0\) of hyperbolas are orthogonal to each other, thus these families are orthogonal trajectories to each other.
Similarly, \(uv=c;c\neq 0 \) and \( u^2-v^2=c;c\neq 0\) are orthogonal to each other on the surface, so these families are orthogonal trajectories to each other.


Next, the family of circles \(x^2+y^2=c\) and that of lines \(y=mx\) are orthogonal trajectories to each other.
Similarly, \(u^2+v^2=c \) and \( v=mu\) are orthogonal to each other on the surface, so these families are orthogonal trajectories to each other.

Differential equation of orthogonal trajectories

Let S: \(\vec{r}=\vec{r}(u,v) \) be a surface. If
\( \phi(u,v)=c\) (i) be a family of curves with directions (du,dv)
\( \psi(u,v)=c_1\) (ii)be another family of curves with directions (-Q,P)
Then, the families (i) and (i) are orthogonal trajectories if (du,dv) and (-Q,P) are orthogonal.
Then, differential equation of orthogonal trajectories is
\(Ell'+F(lm'+l'm))+Gmm'=0\)
or \(Edu(-Q)+F(Pdu-Qdv)+GPdv=0\)
or \((FP-EQ)du+(GP-FQ)dv=0 \)




Family of Curves

MEAN






Family of Curves

Let S: \(\vec{r}=\vec{r}(u,v)\) be a surface and
\( \phi(u,v)=c\) (i)
be a single valued function of \((u,v)\) having continuous derivatives \( \phi_1\) and \( \phi_2\) which do not vanish together. Then an equation (i) where c is real parameter gives a family of curves lying on the surface.
For different values of c, (i) gives different curves on the surface.

Example

  1. As we know \( x^2+y^2=c\); where c is a real parameter represent a family of circles
    Similarly, \( u^2+v^2=c\); where c is a real parameter represent a family of circles on the surface\)

  2. As we know \( y=mx\); where m is real parameter represent a family of straight
    Similarly, \( v=mu\); where m is a real parameter represent a family of curves on the surface

  3. As we know, \(xy=c;c \ne 0\); where c is real parameter represent a family hyperbola
    Similarly, \( uv=c\); where c is a real parameter represent a family of curves on the surface

  4. As we know, \(x^2-y^2=c;c\neq 0\); where c is real parameter represent another family hyperbolas
    Similarly, \( u^2-v^2=c\); where c is a real parameter represent a family of curves on the surface

Differential equation of family of curves

Let S: \(\vec{r}=\vec{r}(u,v)\) be a surface and \( \phi(u,v)=c\) be a family of curves, then
\( \phi(u,v)=c\)
or\( \phi_1 du+\phi_2 dv=0 \)
or\(\frac{du}{dv}=- \frac{\phi_2}{\phi_1} \)
or\(\frac{du}{dv}=- \frac{Q}{P} \) where \((-\phi_2,\phi_1) \) are proportional to (-Q,P)
is called differential equation of family of curves.




Direction coefficients and related results

MEAN







Let S:\(\vec{r}=\vec{r}(u,v)\) be a surface.
Then tangent line to the surface is described by
\( \vec{T}=\lambda \vec{r}_1+\mu \vec{r}_2 \)
Here
\( (\lambda, \mu )\) is called direction components
If \( \vec{e} \) is unit vector along this tangent line, then
\( \vec{e}=l \vec{r}_1+m\vec{r}_2\)
Here
\( (l, m )\) is called direction coefficients
in which
\( El^2+2Flm+Gm^2=1\)

Relation between \( (\lambda,\mu)\) and \( (l,m) \)

Let S:\(\vec{r}=\vec{r}(u,v)\) be a surface with direction components \( (\lambda, \mu )\) and direction coefficients \( (l, m )\) then
\( \frac{l}{\lambda},\frac{m}{\mu} =k \), (say)
or \( l=\lambda k, m= \mu k\)

Now,
\( El^2+2Flm+Gm^2=1\)
or\( E(\lambda k)^2+2F(\lambda k)(\mu k)+G(\mu k)^2=1\)
or\( k^2 (E \lambda ^2+2F \lambda \mu +G \mu^2) =1\)
or \( k=\frac{1}{\sqrt{E \lambda ^2+2F \lambda \mu +G \mu^2}}\)
Thus,
\( (l, m )= \left ( \frac{\lambda}{\sqrt{E \lambda ^2+2F \lambda \mu +G \mu^2}},\frac{\mu}{\sqrt{E \lambda ^2+2F \lambda \mu +G \mu^2}} \right )\)

Direction coefficients of parametric curves

Let S:\(\vec{r}=\vec{r}(u,v)\) be a surface with parametric curves
u=constant (v-curve) and v=constant (u-curve).
Then, \(\vec{r}_1\) is tangent to v= constant curve, thus
\(\vec{r}_1=1\cdot \vec{r}_1+0\cdot \vec{r}_2\)
Here, component of \(\vec{r}_1\) is (1,0), so direction coefficient of v= constant curve (u-curve) is
\((l,m)= \left ( \frac{\lambda}{\sqrt{E \lambda ^2+2F \lambda \mu +G \mu^2}},\frac{\mu}{\sqrt{E \lambda ^2+2F \lambda \mu +G \mu^2}} \right )\)
or\((l,m)= \left ( \frac{1}{\sqrt{E}},0 \right )\)
Similarly,
we know that, \(\vec{r}_2\) is tangent to u= constant curve (v-curve), thus
\(\vec{r}_2=0 \cdot \vec{r}_1+1 \cdot \vec{r}_2\)
Here, component of \(\vec{r}_2\) is (0,1), so direction coefficient of u= constant curve (v-curve) is
\((l,m)= \left ( \frac{\lambda}{\sqrt{E \lambda ^2+2F \lambda \mu +G \mu^2}},\frac{\mu}{\sqrt{E \lambda ^2+2F \lambda \mu +G \mu^2}} \right )\)
or\((l,m)= \left ( 0,\frac{1}{\sqrt{G}} \right )\)

Angle between two directions

Let S: \(\vec{r}=\vec{r}(u,v)\) be a surface \( (l,m)\) and \( (l' ,m')\) be two direction at P, then their corresponding unit vectors are
\( \vec{e} = l\vec{r}_1+m \vec{r}_2 \)
\( \vec{e}' = l' \vec{r}_1+m' \vec{r}_2 \)
If θ be the angle between these directions then
\( \cos \theta = \vec{e}. \vec{e}' \)
or \( \cos \theta = (l\vec{r}_1+m \vec{r}_2) . ( l' \vec{r}_1+m' \vec{r}_2 ) \)
or \( \cos \theta = Ell'+F(lm'+l'm)+Gmm' \)
Also
\( \sin \theta = | \vec{e} \times \vec{e}' | \)
or \( \sin \theta = |(l\vec{r}_1+m \vec{r}_2) \times ( l' \vec{r}_1+m' \vec{r}_2 )| \)
or \( \sin \theta =H(lm'-l'm) \)
Therefore
\( \tan \theta = \frac{H(lm'-l'm)}{Ell'+F(lm'+l'm)+Gmm'} \)
Note
If two directions \( (l,m)\) and \( (l' ,m')\) are orthogonal, then
\( Ell'+F(lm'+l'm)+Gmm'=0 \)
or \( E \frac{l}{m} \frac{l'}{m'}+F \left (\frac{l}{m} + \frac{l'}{m'} \right )+G'=0 \)
Equivalently, if two directions \( (\lambda,\mu)\) and \( (\lambda' ,\mu')\) are orthogonal, then
\( E \lambda \lambda '+F(\lambda \mu '+\lambda ' \mu)+G \mu \mu'=0 \)
or \( E \frac{\lambda}{\mu} \frac{\lambda'}{\mu'}+F \left (\frac{\lambda}{\mu} + \frac{\lambda'}{\mu'} \right )+G'=0 \)




Fundamental Cofficients of Surface

MEAN






Some Common Example of Surface
  1. Plane surface

    Plane is a surface traced by a straight line whose parameters are of degree 1. One example of plane surface is given by
    \( \vec{r}=(u, v,u+v) \)
  2. Cylinder

    Cylinder is a surface traced by a straight line being parallel to a fixed vector. It is given by an equation
    \( \vec{r}=(r \cos u, r \sin u,v) \)
  3. Cone

    Cone is a surface traced by a straight line being fixed to a fixed point. It is given by an equation
    \( \vec{r}=(v \cos u, v \sin u,v) \)
  4. Paraboloid
    \(\vec{r}=( u,v,u^2+v^2 ) \)
  5. Hyperboloid
    \( \vec{r}=(x,y,x^2-y^2) \)
  6. Minimal surface
    \( \vec{r}=(x,y,\log \cos y-\log \cos x) \)
  7. The helicoid
    \( \vec{r}=(u \cos v,u \sin v ,v) \)
  8. Pseduo-sphere
    \(\vec{r}=(\sec h u \cos v, \sec h u \sin v, u-\tan h )\)
  9. Monge’s form
    \( \vec{r}=( u,v,f( u,v ) )\)
  10. Surface of revolution
    \(\vec{r}=(u \cos v,u \sin v, f( u ))\)
  11. Conoidal surface
    \( \vec{r}=( u \cos v,u \sin v,f( v ) ) \)
  12. Saddle surface
    \( \vec{r}=( u,v,uv) \)



Compute Fundamental Cofficients of surface

Compute fundamental coefficients for a saddle surface \( \vec{r}=(u,v,uv) \)
Solution
The saddle surface is
\( \vec{r}=(u,v,uv) \)(i)
Differentiation of (i) w. r. to. u and v, we get
\( \vec{r}_1=(1,0,v) \)
\( \vec{r}_2=(0,1,u) \)
\( \vec{r}_{11}=(0,0,0) \)
\( \vec{r}_{12}=(0,0,1) \)
\( \vec{r}_{22}=(0,0,0) \)
Here, we used the suffix 1 and 2 for derivatives with respect to u and v and respectively, and similarly for higher derivatives.
Now, first order fundamental coefficients are
\( E=\vec{r}_1^2=(1,0,v)^2=1+v^2 \)
\( F=\vec{r}_1. \vec{r}_2=(1,0,v).(0,1,u)=uv \)
\( G=\vec{r}_2^2=(1,0,u)^2=1+u^2 \)
Next,we have to compute second fundamental cofficients,for this
\( H\vec{N}=\vec{r}_1\times \vec{r}_2 \)
or \( H\vec{N}=(1,0,v)\times (0,1,u) \)
or \( H\vec{N}=(-v,-u,1) \) (A)
Taking magnitude, we get
\( H=\sqrt{1+u^2+v^2}\)
And substituting H in (A) we get
\( \vec{N}=\frac{(-v,-u,1)}{\sqrt{1+u^2+v^2}}\)
Hence, the second order fundamental coefficients are
\(L= \vec{r}_{11}.\vec{N}=(0,0,0).\frac{(-v,-u,1)}{\sqrt{1+u^2+v^2}}=0\)
\(M= \vec{r}_{12}.\vec{N}=(0,0,1).\frac{(-v,-u,1)}{\sqrt{1+u^2+v^2}}=\frac{1}{\sqrt{1+u^2+v^2}}\)
\(N= \vec{r}_{22}.\vec{N}=(0,0,0).\frac{(-v,-u,1)}{\sqrt{1+u^2+v^2}}=0\)
This completes the solution


Find fundamental coefficients of following surface

  1. Monge’s form: \( \vec{r}=( x,y,f( x,y ) )\)

    Answer:
    \( \vec{N}=\left\{-\frac{f_1}{\sqrt{1 + f_1^2 + f_2^2}}, -\frac{f_2}{\sqrt{1 + f_1^2 + f_2^2}}, \frac{1}{\sqrt{1 + f_1^2 + f_2^2}}\right\} \)
    Cofficients: \( \left\{1 + f_1^2, f_1 f_2, 1 + f_2^2, \frac{f_{11}}{\sqrt{1 + f_1^2 + f_2^2}}, \frac{f_{12}}{\sqrt{1 + f_1^2 + f_2^2}}, \frac{f_{22}}{\sqrt{1 + f_1^2 + f_2^2}}\right\} \)

  2. Surface of revolution: \(\vec{r}=( u \cos v,u \sin v,f( u ) )\)

    Answer:
    \( \vec{N}=\left\{-\frac{f_1 u \cos v}{H}, -\frac{f_1 u \sin v}{H}, \frac{u}{H}\right\} \)
    Cofficients: \( \left\{1 + f_1^2, 0, u^2, \frac{f_{11} u}{H}, 0, \frac{f_1 u^2}{H}\right\} \)

  3. Conoidal surface:\( \vec{r}=( u \cos v,u \sin v,f( v ) ) \)

    Answer:
    \( \vec{N}=\left\{\frac{f_2 \sin v}{H}, -\frac{f_2 \cos v}{H}, \frac{u}{H}\right\}\)
    Cofficients: \( \left\{1, 0, f_2^2 + u^2, 0, -\frac{f_2}{H}, \frac{f_{22} u}{H}\right\} \)

  4. Right helicoid: \( \vec{r}=( u \cos v,u\sin v,cv ) \)

    Answer:
    \( \vec{N}=\left\{\frac{c \sin v}{H}, -\frac{c \cos v}{H}, \frac{u}{H}\right\}\)
    Cofficients: \( \left\{1, 0, c^2 + u^2, 0, -\frac{c}{H}, 0\right\} \)

  5. Plane surface: \( \vec{r}=( u,v,u+v) \)

    Answer:
    \( \vec{N}=\left\{\frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}}, 0\right\}\)
    Cofficients: \( \{3, 1, 1, 0, 0, 0\} \)

  6. Saddle surface: \( \vec{r}=( u,v,uv) \)

    Answer:
    \( \vec{N}=\left\{-\frac{v}{\sqrt{1 + u^2 + v^2}}, -\frac{u}{\sqrt{1 + u^2 + v^2}}, \frac{1}{\sqrt{1 + u^2 + v^2}}\right\}\)
    Cofficients: \( \left\{1 + v^2, uv, 1 + u^2, 0, \frac{1}{\sqrt{1 + u^2 + v^2}}, 0\right\}\)

  7. Saddle surface: \( \vec{r}=( u+v,u-v,uv ) \)

    Answer:
    \( \vec{N}=\left\{\frac{u + v}{\sqrt{2} \sqrt{2 + u^2 + v^2}}, \frac{-u + v}{\sqrt{2} \sqrt{2 + u^2 + v^2}}, -\frac{\sqrt{2}}{\sqrt{2 + u^2 + v^2}}\right\} \)
    Cofficients: \( \left\{2 + v^2, uv, 2 + u^2, 0, -\frac{\sqrt{2}}{\sqrt{2 + u^2 + v^2}}, 0\right\}\)

  8. Paraboloid:\(\vec{r}=( u,v,u^2+v^2 ) \)

    Answer:
    \( \vec{N}=\left\{\frac{v}{\sqrt{2}}, -\frac{v}{\sqrt{2}}, 0\right\}\)
    Cofficients: \( \{a^2, 0, 1, -a, 0, 0\} \)

  9. Cylinder: \( \vec{r}=(a\cos u, a\sin u,v ) \)

    Answer:
    \( \vec{N}=\{\cos u, \sin u, 0\}\)
    Cofficients: \( \{2 + 4 u^2, 4 u v, 4 v^2, 0, 0, 0\} \)

  10. Cone: \( \vec{r}=(v\cos u, v\sin u,v ) \)

    Answer:
    \( \vec{N}=\left\{\frac{v \cos u}{\sqrt{2}}, \frac{v \sin u}{\sqrt{2}}, -\frac{v}{\sqrt{2}}\right\} \)
    Cofficients: \( \left\{v^2, 0, 2, -\frac{v^2}{\sqrt{2}}, 0, 0\right\} \)

  11. Sphere: \( \vec{r}=(\sin u \cos v,\sin u \sin v, \cos u) \)

    Answer:
    \( \vec{N}=\left\{\frac{\cos v \sin^2 u}{H}, \frac{\sin^2 u \sin v}{H}, \frac{\cos u \sin u}{H}\right\} \)
    Cofficients: \( \left\{1, 0, \sin^2 u, -\frac{\sin u}{H}, 0, -\frac{\sin^3 u}{H}\right\} \)

  12. Hyperboloid: \( 2z=7x^2+6xy-y^2 \)at origin

    Answer:
    \( \vec{N}= \{0,0,1\}\)
    Cofficients: \( \left\{ 1,0,1,7,3,-1\right\} \)

  13. Minimal surface: \( e^z \cos x=\cos y \)

    Answer:
    \( \vec{N}= \left\{-\frac{\tan x}{H}, \frac{\tan y}{H}, \frac{1}{H}\right\} \)
    Cofficients: \( \left\{\sec^2 x, -\tan x \tan y, \sec^2 y, \frac{\sec^2 x}{H}, 0, -\frac{\sec^2 y}{H}\right\} \)




Fundamental Forms of Surface

MEAN



We recall that, space curve is uniquely determined by two local invariant quantities: curvature and torsion.Similarly, surface is uniquely determined by two local invariant quantities: first and second fundamental form of surface




First Fundamental Form of Surface







Let \( S:\vec{r}=\vec{r}( u,v ) \) be a surface, then, quadratic differential form in \( du,dv \) given by
\( I:Edu^2+2Fdudv+Gdv^2 \) where \( E=\vec{r_1}^2,F=\vec{r}_1.\vec{r}_2,G=\vec{r}_2^2 \)
is called first fundamental form of the surface. The coefficients \( E,F,G\) are called the first fundamental coefficients or magnitude of first order.




Geometry of First Fundamental Form of Surface

  

Let \( S:\vec{r}=\vec{r}( u,v ) \) be a surfacein which \( P \) and \( Q \) are two neighboring points with
\( \overrightarrow{OP}=\vec{r} \) and \( \overrightarrow{OQ}=\vec{r}+d\vec{r}\)
Then
\( \overrightarrow{PQ}=\overrightarrow{OQ}-\overrightarrow{OP} \)
or \( d\vec{r}=\vec{r}( u+du,v+dv )-\vec{r}( u,v) \)
or \( d\vec{r}=\vec{r}( u,v )+( \vec{r}_1du+\vec{r}_2dv )+\frac{1}{2!}(\vec{r}_1du+\vec{r}_2dv )^2+...-\vec{r}( u,v ) \)
or \( d\vec{r}=( \vec{r}_1du+\vec{r}_2dv )+\frac1{2!}{{( \vec{r}_1du+\vec{r}_2dv )}^2}+\ldots \)
The first order approximation is
\(dr=( \vec{r}_1du+\vec{r}_2dv ) \)
Squaring on both sides, we get
\( ds^2=(\vec{r}_1du+\vec{r}_2dv )^2 \)
or \( ds^2=\vec{r}_1^2du^2+2\vec{r}_1\vec{r}_2dudv+\vec{r}_2^2dv^2 \)
or \( ds^2=Edu^2+2Fdudv+Gdv^2\) where \( E=\vec{r}_1^2,F=\vec{r}_1.\vec{r}_2,G=\vec{r}_2^2 \)

Note
  1. For \( u\) curve \( ds^2=Edu^2 \)
  2. For \( v \) curve \( ds^2=Gdv^2 \)



By the ordinary property of vector operation,
\( ( \vec{r}_1\times \vec{r}_2)^2=\vec{r}_1^2. \vec{r}_2^2-( \vec{r}_1.\vec{r}_2 )^2 \)
or \( (H \vec{N})^2=E.G-F^2 \)
or \(H^2=E.G-F^2 \), which is always positive.







Property 1 : First Fundamental Form is Positive

The first fundamental form of the surface is positive definite in \( du \) and \( dv \).
Proof
Let \(S:\vec{r}=\vec{r}( u,v ) \) be a surface, then
\( H^2=E.G-F^2 \) is always positive
Now, assume that \( E >0 \), then
\(I=Edu^2+2Fdudv+Gdv^2 \)
or \(I=\frac{1}{E}( E^2du^2+2EFdudv+EGdv^2 )\)
or \(I=\frac{1}{E}[ ( Edu+Fdv )^2+( EG-F^2 )dv^2 ]\)
or \(I=\frac{1}{E}[ ( Edu+Fdv )^2+H^2dv^2 ]\)
Here, \(I \) has two possibilities, one is \( I=0 \) and other is \( I>0 \)
If possible, suppose that
\( I=0 \)
Then, we must have
\( \frac{1}{E}[ ( Edu+Fdv )^2+H^2dv^2 ]=0 \)
or \( ( Edu+Fdv )^2+H^2dv^2=0 \)
or \( ( Edu+Fdv )^2=0 \) and \( H^2 dv^2=0 \)
or \( ( Edu+Fdv )^2=0 \) and \( dv^2=0 \)
or \(Edu+Fdv=0 \) and \( dv=0 \)
or \(Edu =0 \) and \( dv=0 \)
or \( du=0 \) and \( dv= 0 \) , which is not possible.
Hence, first fundamental form is positive definite in \( du \) and \( dv \).




Property 2 : First Fundamental Form is Invariant

The first fundamental form is invariant under parametric transformation.
Proof
Let \( S:\vec{r}=\vec{r}( u,v ) \) be a surface, and parameters \( ( u,v ) \) is transformed into another set \(( U,V ) \) set of parameters such that
\(U =\phi ( u,v ) \) and \( V=\psi ( u,v ) \)
Now
\(I = Edu^2+2Fdudv+Gdv^2 \) where \( E=\vec{r}_1^2,F=\vec{r}_1.\vec{r}_2,G=\vec{r}_2^2 \)
or \( I =(\textcolor{red}{ \vec{r}_1} du+ \textcolor{red}{ \vec{r}_2} dv )^2 \)
or \( I =( \textcolor{red}{ \frac{\partial \vec{r}} {\partial u}} du + \textcolor{red}{ \frac{\partial \vec{r}} {\partial v}} dv)^2 \)
or \(I = ( [ \textcolor{red}{ \frac{\partial \vec{r}} {\partial U} \frac{\partial U} {\partial u} + \frac{\partial \vec{r}} {\partial V} \frac{\partial V} {\partial u} } ] du + [ \textcolor{red}{ \frac{\partial \vec{r}} {\partial U} \frac{\partial U} {\partial v} + \frac{\partial \vec{r}} {\partial V} \frac{\partial V} {\partial v} }] dv)^2 \)
or \(I = ( \frac{\partial \vec{r}} {\partial U} \frac{\partial U} {\partial u} du + \frac{\partial \vec{r}} {\partial V} \frac{\partial V} {\partial u} du + \frac{\partial \vec{r}} {\partial U} \frac{\partial U} {\partial v} dv + \frac{\partial \vec{r}} {\partial V} \frac{\partial V} {\partial v} dv)^2 \)
or \(I = ( \frac{\partial \vec{r}} {\partial U} \frac{\partial U} {\partial u} du +\frac{\partial \vec{r}} {\partial U} \frac{\partial U} {\partial v} dv + \frac{\partial \vec{r}} {\partial V} \frac{\partial V} {\partial u} du + \frac{\partial \vec{r}} {\partial V} \frac{\partial V} {\partial v} dv)^2 \)
or \(I = ( \frac{\partial \vec{r}} {\partial U} [\frac{\partial U} {\partial u} du + \frac{\partial U} {\partial v} dv] + \frac{\partial \vec{r}} {\partial V} [ \frac{\partial V} {\partial u} du + \frac{\partial V} {\partial v} dv])^2 \)
or \(I = ( \frac{\partial \vec{r}} {\partial U}dU + \frac{\partial \vec{r}} {\partial V}dV)^2 \)
or \(I = EdU^2+2FdU dV+GdV^2 \) where \( E= (\frac{\partial \vec{r}} {\partial U})^2,F=\frac{\partial \vec{r}} {\partial U}.\frac{\partial \vec{r}} {\partial V},G= (\frac{\partial \vec{r}} {\partial V})^2 \)
This shows that, first fundamental form is invariant under parametric transformation.




Elements of surface area

  

Let \(S:\vec{r}=\vec{r}( u,v )\) be a surface. If \(\Delta R=PQRS\) is a small region on the surface with
\(P( u,v ),Q( u+du,v ),R( u+du,v+dv )\) and \(( u,v+dv ) \).
Then, \( PQRS \) tends to a parallelogram when \( du, dv \) are very small and positive
Thus
Area of \( PQRS =| \vec{PQ} \times \vec{PS} | \) (i)
Here
\( \vec{PQ}=\vec{OQ}-\vec{OP} \)
or \( \vec{PQ}=\vec{r}( u+du,v )-\vec{r}( u,v ) \)
or \( \vec{PQ}=\vec{r}( u,v )+\vec{r}_1du+... -\vec{r}( u,v ) \)
Taking first order approximation, we get
\( \vec{PQ}=\vec{r}_1du \) (ii)
Similarly we get
\( \vec{PS}=\vec{r}_2dv \) (iii)
Thus, from (i), (ii) and (iii), we have
Area of \( PQRS = | \vec{r}_1 du \times \vec{r}_2dv | \)
or Area of \( PQRS =| \vec{r}_1 du \times \vec{r}_2 dv | \)
or Area of \( PQRS =| \vec{r}_1 \times \vec{r}_2 | du dv\)
or Area of \( PQRS =H du dv\)




Second Fundamental Form of the Surface

Let \(S:\vec{r}=\vec{r}( u,v )\) be a surface.Then quadratic differential form in \( du, dv \)
\( II:Ldu^2+2Mdudv+Ndv^2 \) where \(L=\vec{r}_{11}.\vec{N},M=\vec{r}_{12}.\vec{N},N=\vec{r}_{22}.\vec{N} \)
is called second fundamental form of the surface.
The coefficients \(L,M,N \) are called the second fundamental coefficients or magnitude of second order.






Geometry of Second Fundamental Form of the Surface

Length of perpendicular on the tangent plane from neighborhood point on the surface is
\(\frac12( Ldu^2+2Mdudv+Ndv^2 ) \)
Proof
Let \( S:\vec{r}=\vec{r}( u,v ) \) be a surfacein which \( P \) and \( Q \) are two neighboring points with
\( \vec{OP}=\vec{r} \) and \( \vec{OQ}=\vec{r}+d\vec{r}\)
Then
\( \vec{PQ}=\vec{OQ}-\vec{OP} \)
or \( d\vec{r}=\vec{r}( u+du,v+dv )-\vec{r}( u,v) \)
or \( d\vec{r}=\vec{r}( u,v )+( \vec{r}_1du+\vec{r}_2dv )+\frac{1}{2!}( \vec{r}_1du+\vec{r}_2dv )^2+...-\vec{r}( u,v ) \)
or \( d\vec{r}=( \vec{r}_1du+\vec{r}_2dv )+\frac{1}{2!}( \vec{r}_1du+\vec{r}_2dv )^2+... \)
The second order approximation is
\( d\vec{r}=( \vec{r}_1du+\vec{r}_2dv )+\frac{1}{2!}( \vec{r}_1du+\vec{r}_2dv )^2 \)
or \( d\vec{r}= (\vec{r}_1du+\vec{r}_2dv )+ \frac{1}{2} ( \vec{r}_{11} du^2 +2 \vec{r}_{12} du dv+ \vec{r}_{22} dv^2) \)
Now, let M be the projection of Q on the tangent plane at P, then
\( QM=\) Projection of \( \vec{PQ} \) on the normal at P
or \( QM=\vec{PQ}.\vec{N}\)
or \( QM=[ ( \vec{r}_1du+\vec{r}_2dv )+\frac{1}{2!}( \vec{r}_{11}du^2+2\vec{r}_{12}dudv+\vec{r}_{22}dv^2 ) ].\vec{N} \)
or \( QM=\frac{1}{2!}( \vec{r}_{11}.\vec{N}du^2+2\vec{r}_{12}.\vec{N}dudv+\vec{r}_{22}.\vec{N}dv^2 )\)
or \( QM=\frac{1}{2}( Ldu^2+2Mdudv+Ndv^2 )\) where \(L=\vec{r}_{11}.\vec{N},M=\vec{r}_{12}.\vec{N},G=\vec{r}_{22}.\vec{N} \)




Alternative forms of \( L, M, N \)


As we know that \(\vec{r_1}\) is tangent to u-curve; and \(\vec{r_2}\) is tangent to v-curve, so \(\vec{r_1}\) and \(\vec{r_2}\) are tangents of the surface \( S:\vec{r}=\vec{r}( u,v ) \). Therefore, \(\vec{r_1}\) and \(\vec{r_2}\) ate perpendicular to the normal vector \(\vec{N}\). Also, we know that \(L=\vec{r}_{11}.\vec{N},M=\vec{r}_{12}.\vec{N},G=\vec{r}_{22}.\vec{N} \). Now, the fundamental coefficients \(L,M,N\) can be alternatively explained as below.
  1. Also, we know that
    \(\vec{r}_1. \vec{N}=0 \)(1)
    Differentiating (1) w. r. to u, we, get
    \(\vec{r}_{11}. \vec{N}+\vec{r}_1. \vec{N}_1=0 \)
    or \(L+\vec{r}_1. \vec{N}_1=0 \)
    or \(\vec{r}_1. \vec{N}_1=-L \)
  2. Also, we know that
    \(\vec{r}_1. \vec{N}=0 \)(1)
    Differentiating (1) w. r. to v, we, get
    \(\vec{r}_{12}. \vec{N}+\vec{r}_1. \vec{N}_2=0 \)
    or \(M+\vec{r}_1. \vec{N}_2=0 \)
    or \(\vec{r}_1. \vec{N}_2=-M \)

  3. Also, we know that
    \(\vec{r}_2. \vec{N}=0 \)(1)
    Differentiating (1) w. r. to u, we, get
    \(\vec{r}_{21}. \vec{N}+\vec{r}_2. \vec{N}_1=0 \)
    or \(M+\vec{r}_2. \vec{N}_1=0 \)
    or \(\vec{r}_2. \vec{N}_1=-M \)

  4. Also, we know that
    \(\vec{r}_2. \vec{N}=0 \)(1)
    Differentiating (1) w. r. to v, we, get
    \(\vec{r}_{22}. \vec{N}+\vec{r}_2. \vec{N}_2=0 \)
    or \(N+\vec{r}_2. \vec{N}_2=0 \)
    or \(\vec{r}_2. \vec{N}_2=-N \)

Based on the cofficients of L, M and N, we can write that
  1. \([\vec{r}_1,\vec{r}_2,\vec{r}_{11}]=\vec{r}_1 \times \vec{r}_2 .\vec{r}_{11}=H \vec{N} .\vec{r}_{11}=HL\)
  2. \([\vec{r}_1,\vec{r}_2,\vec{r}_{12}]=\vec{r}_1 \times \vec{r}_2 .\vec{r}_{12}=H \vec{N} .\vec{r}_{12}=HM\)
  3. \([\vec{r}_1,\vec{r}_2,\vec{r}_{21}]=\vec{r}_1 \times \vec{r}_2 .\vec{r}_{21}=H \vec{N} .\vec{r}_{21}=HM\)
  4. \([\vec{r}_1,\vec{r}_2,\vec{r}_{22}]=\vec{r}_1 \times \vec{r}_2 .\vec{r}_{22}=H \vec{N} .\vec{r}_{22}=HN\)



Nature of points on a surface

The second fundamental form of a surface measures osculation paraboloid, which helps to determines nature of points on the surface. These points are as follows
  1. Case 1: Parabolic
    A point on a surface is called parabolic point if
    \(LN-M^2=0;L^2+M^2+N^2 \ne 0\)
    In parabolic point, there exists a line in tangent plane whose normal curvature is zero. So, at this point, exactly one of principal curvatures \(K_1\) and \(K_2\) is zero. Since one normal curvature is zero, the direction corresponding to the zero principal curvature will be the direction of the asymptotic curve. The nbd point of the surface lies on same side of the tangent plane. An example of such point is shown in a paraboloid cylinder in figure.
  2. Case 2: Hyperbolic
    A point is called hyperbolic point if
    \(LN-M^2<0\)
    In hyperbolic point, there exists two lines in tangent plane whose normal curvatures: \(K_1\) and \(K_2\) have opposite sign. In such point, there exists two asymptotic direction. The nbd point of the surface lies on both sides of the tangent plane. An example of such point is shown in a hyperboloid surface in figure
  3. Case 3: Elliptic
    A point is called elliptic point if
    \(LN-M^2>0\)
    In elliptic point, there exists tangent plane whose normal curvatures: \(K_1\) and \(K_2\) have same sign. In such point, there exists no asymptotic direction. The nbd point of the lies on same side of the tangent plane. An example of such point is shown in an elliptic surface in figure
  4. Case 4: Planner
    A point is called planner point if
    \(LN-M^2=0;L^2+M^2+N^2= 0\)
    If \(L,M,N\) and \(LN-M^2\) are all zero, then surface is planar, means both of \(K_1\) and \(K_2\) is zero.



Tuesday, August 6, 2024

Equations of tangent and normal to a parabola

MEAN
📘






Tangent to Parabola at \( (x_1, y_1) \)

Answer 👉 Click Here




Condition of Tangenncy to Parabola

Answer 👉 Click Here




Normal to Parabola at \( (x_1, y_1) \)

Answer 👉 Click Here




Tangent and Normal to Parabola in Parametric Form

Answer 👉 Click Here




Exercise

  1. Find the equation of tangent and normal to the parabola
    1. \( y^2=8x\) at (2,-4)

      Answer 👉 Click Here

    2. \( x^2=12y\) at (-6,3)

      Answer 👉 Click Here

    3. \( x^2=4y\) at the point whose abscissa is 6

      Answer 👉 Click Here

    4. \( y^2=16ax\) at the point whose ordinate is -4a

      Answer 👉 Click Here

    5. \( y^2=12x\) at each end of the latus rectum

      Answer 👉 Click Here

  2. Solve the followings
    1. Prove that the line \(3x+4y+6=0\) is tangent to the parabola \(2y^2=9x\) and find its point of contact

      Answer 👉 Click Here

    2. Prove that the line \(lx+my+n=0\) touches the parabola \(y^2=4ax\) if \(ln =am^2\)

      Answer 👉 Click Here

    3. For what value of a, will the straight line \(y=2x+3\) touch the parabola \(y^2=4ax\)

      Answer 👉 Click Here

    4. If the line \(2x+4y=3\) touches the parabola \(y^2=4ax\) find the length of the latus rectum

      Answer 👉 Click Here

  3. Solve the followings
    1. Find the equation of tangent to the parabola \(y^2=4x\)
      (i) parallel to the line \(x-2y+6=0\).
      (ii) perpendicular to the line \(2x-y=4\)
      Also find the point of contact.

      Answer 👉 Click Here

    2. Find the rquation of normal line to the parabola \(y^2=3x\)
      (i) parallel to the line \(y=2x+1\)
      (ii) perpendicular to the line \(3x+2y=8\)

      Answer 👉 Click Here

  4. Solve the followings
    1. Show that tangent to the parabola \(y^2=4x\) and \(x^2=4y\) at (1,2) and (-2,1) respectively are at right angles.

      Slope of the tangent to the Parabola \( y^2 = 4x \) at \( (1, 2) \)is
      \( m_1 = \frac{y_1}{2a} \)
      \( m_1 = \frac{2}{2} = 1 \)
      Next, slope of the tangent to the Parabola \( x^2 = 4y \) at \( (-2, 1) \)is
      \( m_2 = \frac{x_1}{2a} \)
      \( m_2 = \frac{-2}{2} = -1 \)
      The tangents are perpendicular if the product of their slopes is \(-1\).
      \( m_1 \times m_2 = 1 \times -1 = -1 \)
      Since the product of the slopes is \(-1\), the tangents are at right angles
    2. Show that normal to the parabola \(y^2=8x\) at (2,4) meets the parabola again in (18,-12)

      The equation of the parabola is \( y^2 = 8x \), so the slope of normal to the parabola is
      \( m= -\frac{2a}{y_1} \)
      \( m= - \frac{2.2}{4} = -1 \)
      Now, equation of the Normal at \( (2, 4) \) is
      \( y - y_1 = m(x - x_1) \)
      \( y - 4 = -1(x - 2) \)
      \( y = -x + 6 \)
      \( x + y - 6 = 0 \)
      To find where the normal meets the parabola again, substitute the equation of the normal \( x + y - 6 = 0 \) into the equation of the parabola \( y^2 = 8x \), we get
      \( y^2 = 8x \)
      \( (6 - x)^2 = 8x \)
      \( 36 - 12x + x^2 = 8x \)
      \( x^2 - 20x + 36 = 0 \)
      \( x = 2 \) or \( x = 18 \)
      When \( x = 2 y = 4 \) is the original point, and when \( x = 18 \), we get \( y = 6 - 18 = -12 \).
      Therefore, the normal meets the parabola again at \( (18, -12) \)
  5. Solve the followings
    1. Find the equation of tangent to the parabola \(y^2=6x\) making angle 45 degree with the x-axis. Also find the point of contact.

      Given that, parabola is \(y^2=6x\), thus,
      \( 4a = 6\) gives \(a=\frac{3}{2}\)
      Also, given that tangent makes an angle of 45 degrees with the x-axis. Therefore, the slope \(m\) of the tangent is
      \( m = \tan(45^\circ) = 1 \)
      Now, the equation of the tangent to the parabola \( y^2 = 4ax \) is
      \( y=mx+\frac{a}{m}\)
      \( y = 1.x + \frac{3}{2} \)
      \( y = x + \frac{3}{2} \)
      To find the point of contact, we substitute the tangent equation \( y = x +\frac{3}{2}\) into the parabola equation \( y^2 = 6x \), so we get
      \( y^2 = 6x \)
      \( (x + \frac{3}{2})^2 = 6x \)
      \( (2x + 3)^2 = 24x \)
      \( (2x - 3)^2 = 0 \)
      \( x= \frac{3}{2}\) gives \( y = \frac{3}{2} + \frac{3}{2} =3\)
      Hence, the point of contact is \( (\frac{3}{2},3)\).
    2. A tangent to the parabola \(y^2=12x\) makes an angle 45 degree with the straight line \(2y=x+3\). Find its equation and point of contact.
    3. Find the equation of tangents to the parabola \(y^2=12x\) drawn through the points (-1,2). Also find the point of contact and the angle between two tangents.
    4. Find the equation of common tangents to the parabolas \( y^2=4x\) and \( x^2=4y\)
  6. Solve the followings
    1. Show that the pair of tangents drawn from the point (-2,3) to the parabola \(y^2=8x\) are at right angle
    2. Prove that the tangents at the extrimities of the latus rectum of a parabola \(y^2=16x\) are at right angles

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