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Exercises 1.8 Exercise

1.

Prove that the line joining the midpoints of two sides of a triangle is parallel and half to the third.

2.

A particle is displaced from the point whose position vector is \(5\hat{i}-5\hat{j}-7\hat{k}\) to the point whose position vector is \(6\hat{i}+2\hat{j}-2\hat{k}\) under the action of a number of constant forces defined by \(10\hat{i}-\hat{j}+11\hat{k}\text{,}\) \(4\hat{i}+5\hat{j}+6\hat{k}\text{,}\) and \(-2\hat{i}+\hat{j}-8\hat{k}\text{.}\) Find the work done.
Answer.
92.

3.

A force is represented in magnitude and direction by the line joining the point A(1,-2,4) to the point B(5,2,3). Find its moment about the point (-2,3,5).
Answer.
\begin{equation*} 9\hat{i}-\hat{j}+32\hat{k}. \end{equation*}

4.

A rigid body is rotating at the rate of 2.5 radians per second about an axis AB, where A and B are the points (1,-2,1) and (3,-4,2). Find the velocity of the point P at (5,-1,1) of the body.
Answer.
\begin{equation*} \frac{2.5}{3}[3\hat{i}+8\hat{j}+10\hat{k}] \end{equation*}

5.

A particle P is moving on a circle of radius \(r\) with constant angular velocity \(\omega = \frac{d\theta}{dt}\text{.}\) Show that its acceleration is \(-\omega^{2}\vec{r}\text{.}\)

6.

If \(\phi=log\mid r \mid\text{,}\) then show that \(grad \phi=\frac{\vec{r}}{r^{2}}\text{.}\)

7.

Prove that \(grad \frac{1}{r}=-\frac{r}{r^{3}}\text{.}\)

8.

If \(\phi(x,y,z)=3x^{2}z-xy^{3}+5\text{,}\) find \(\phi\) at the point (a) (0,0,0) and (b) (1,-2,2).
Answer.
(a) 5 and (b) 19.

9.

Find the directional derivative of \(x^{2}+y^{2}+4xy\) at (1,-2,2) in the direction \((2\hat{i}-2\hat{j}+\hat{k})\text{.}\)
Answer.
-44/3.

10.

The temperature of the points in room is given by \(T(x,y,z) = x^{2}+y^{2}-z^{2}\text{.}\) A fly located at (1,1,1) desires to fly in such a direction that it will get warm as soon as possible. In what direction should it fly?
Hint.
Find the unit vector normal to the gradient of a Temperature.
Answer.
\(\frac{1}{2\sqrt{3}}(2\hat{i}+2\hat{j}-2\hat{k})\)

11.

Evaluate \(\vec{\bigtriangledown}\cdot(r^{3}\vec{r})\)
Answer.
\(6r^{3}\)

12.

If \(\vec{A}=\frac{\vec{r}}{r}\text{,}\) find \(\text{grad div} \vec{A}\)
Answer.
\(-2r^{-3}\vec{r}\)

13.

Prove \(\nabla^{2}(\phi \psi) = \phi \nabla^{2}\psi +2\nabla \phi\cdot\nabla \psi +\psi \nabla^{2} \phi\text{.}\)

14.

Prove that the vector \(\vec{A}=3y^{4}z^{2}\hat{i}+4x^{3}z^{2}\vec{j}-3x^{2}y^{2}\hat{k}\) is solenoidal.

15.

If \(\vec{A}\) and \(\vec{B}\) are irrotational, prove that \(\vec{A}\times\vec{B}\) is solenoidal.

16.

Prove that \(\nabla^{2}\left[\nabla\left(\frac{\vec{r}}{r^{2}}\right)\right]= 2r^{-4}\text{.}\)

17.

Find the work done when a force \(\vec{F}=(x^{2}-y^{2}+x)\hat{i}-(2xy+y)\hat{j}\) moves a particle from origin to (1,1) along a parabola \(y^{2}=x\text{.}\)
Answer.
\(\frac{2}{3}\)

18.

Evaluate \(\iint\limits_{R}\sqrt{x^{2}+y^{2}}\,dx\,dy\) over the region R in the xy - plane bounded by \(x^{2}+y^{2}=36\text{.}\)
Answer.
\(144\pi\)

19.

Evaluate \(\iiint\limits_{V}(2x+y) \,dV\text{,}\) where V is the closed region bounded by the cylinder \(z=4-x^{2}\) and the planes \(x=0,y=0,y=2,\) and \(z=0\text{.}\)
Answer.
40.

20.

Use divergence theorem to evaluate \(\iint\limits_{S}\left(y^{2}z^{2}\hat{i}+z^{2}x^{2}\hat{j}+x^{2}y^{2}\hat{k}\right)\cdot\vec{ds}\text{,}\) where S is the upper part of the sphere \(x^{2}+y^{2}+z^{2}=9\) above the x-y plane.
Answer.
\(\frac{243\pi}{8}\)

21.

Verify divergence theorem for \(\vec{F}=4xz\hat{i}+xyz^{2}\hat{j}3z\hat{k}\) over the region above XOY plane bounded by the cone \(z^{2}= x^{2}+y^{2}\) and the plane \(z=4\text{.}\)

22.

Using Stoke’s theorem, evaluate \(\int\limits_{C}[(x+y)dx+(2x-z)dy+(y-z)dz]\text{,}\) where C is the boundary of the triangle with vertices (2,0,0), (0,3,0) and (0,0,6).
Answer.
21.

23.

Represent the vector \(\vec{F}= 2y\hat{i}-z\hat{j}+3x\hat{k}\) in spherical coordinates and determine \(F_{r}, F_{\theta}, F_{\phi}\text{.}\)
Answer.
\begin{equation*} \vec{F} = F_{r}\hat{e}_{r}+F_{\theta}\hat{e}_{\theta}+F_{\phi}\hat{e}_{\phi} \end{equation*}
\begin{equation*} F_{r} = 2y\sin\theta\cos\phi-z\sin\theta\sin\phi+3x\cos\theta \end{equation*}
\begin{equation*} F_{\theta} = 2y\cos\theta\cos\phi-z\cos\theta\sin\phi-3x \end{equation*}
\begin{equation*} F_{\phi} = -2y\sin\phi-z\cos\phi. \end{equation*}

24.

Prove that a spherical coordinate system is orthogonal.

25.

Express the velocity \(\vec{v}\) and acceleration \(\vec{a}\) of a particle in spherical coordinates.
Answer.
\begin{equation*} \vec{v} = v_{r}\hat{e}_{r}+v_{\theta}\hat{e}_{\theta}+v_{\phi}\hat{e}_{\phi}; \end{equation*}
\begin{equation*} \vec{a}= a_{r}\hat{e}_{r}+a_{\theta}\hat{e}_{\theta}+a_{\phi}\hat{e}_{\phi}. \end{equation*}
where, \(v_{r} = \dot{r}, \hspace{4pt} v_{\theta} = r\dot{\theta}, \hspace{4pt} v_{\phi} = r\sin\theta\dot{\phi}\)
\begin{equation*} \text{and} \quad a_{r}=\ddot{r}-r\theta^{2}-r\sin^{2}\theta\dot{\phi}^{2}; \end{equation*}
\begin{equation*} a_{\theta}=\frac{1}{r}\frac{d}{dt}(r^{2}\dot{\theta})-r\sin\theta\cos\phi\dot{\phi}^{2}, \end{equation*}
\begin{equation*} a_{\phi}=\frac{1}{r\sin\theta}\frac{d}{dt}(r^{2}\sin^{2}\theta\dot{\phi}). \end{equation*}