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Problems in Mathematical Analysis.pdf - pwp.net.ipl.pt

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-406 Answers<br />

640. H<strong>in</strong>t. The equation of the tangent is ^-{-^-=1. Hence, the tangent<br />

ZXQ 2yQ<br />

crosses the x-axis at the po<strong>in</strong>t A (2x , 0) and the y-axis at B (0, 2f/ ). F<strong>in</strong>d<strong>in</strong>g<br />

the midpo<strong>in</strong>t of AB, we get the po<strong>in</strong>t (* , yQ ). 643. 40 36'. 644. The para-<br />

bolas are tangent at the po<strong>in</strong>t (0, 0) and <strong>in</strong>tersect at an angle<br />

arctan-i=^88' at the po<strong>in</strong>t (1,1). 647. S,<br />

648 ' ' 652 ' T<br />

653. arc tan ~. 654.<br />

-y +2(p ' 655 ' S = f<br />

* = 2jia /1+4JT 2<br />

rt = 2<br />

a ;<br />

}/~l-|-4ji ; tan^i = 2jt. 656. S, = -- ><br />

t n<br />

a; 5,,= -^;<br />

I<br />

-~ ~ fl2_|_p2. . tan|i= q> 657. 3 cm /sec; 0; 9 cm /sec<br />

658. 15 cm/sec. 659.<br />

g<br />

--x 2 2<br />

K uj<br />

. The<br />

2<br />

-^-<strong>in</strong>/sec. 660. The equation of the trajectory \sy=x tan a<br />

u * s<strong>in</strong> 2a<br />

velocity,<br />

range is -. The<br />

2u g/s<strong>in</strong>a + g 2 / 8 ; the slope of the velocity<br />

vector is<br />

v cosa .<br />

H<strong>in</strong>t. To determ<strong>in</strong>e the trajectory, elim<strong>in</strong>ate the parameter t from the given<br />

system. The range is the abscissa of the po<strong>in</strong>t A (Fig. 17). The projections<br />

of velocity on the axes are ~ and j-<br />

~<br />

The magnitude of the velocity is<br />

' the velocit y vector is directed along the tangent to the<br />

Q<br />

~ ,<br />

CO8<br />

2 f<br />

663. 1 he diagonal <strong>in</strong>creases at a rale ol - '6. 8 cm/sec, the area, at a rate<br />

of 40 cm 2<br />

/sec 664. The surface area <strong>in</strong>creases at a rate of 2ji m 2<br />

/sec,<br />

the volume, at a rate of 0.05 JT m'/'sec. 665. y cm/sec<br />

666. The mass of the rod<br />

is 360 g, the density at M is 5* g/crn, the<br />

density at A is 0, the density<br />

at B is 60g/cm. 667. 56x 6 + 210,Y4 * x<br />

. 668. e (4^ + 2). 669. 2 cos 2x<br />

2(1 ~"* ~~<br />

2)<br />

X<br />

670.<br />

. 671 .<br />

672. 2 arc tan x<br />

2<br />

+<br />

3(1<br />

673. _ + 674 cosh 6 79. y"' = 6. 680. /'"(3)<br />

1 x 2<br />

(1 x*) i* a a<br />

681. y v = ^ .<br />

682.<br />

vl = // ~64s<strong>in</strong>2x 684. 0; 1; 2; 2. 685. The velocity<br />

is u = 5; 4997; 4.7. The acceleration, a = 0; 0.006; 0.6. 686. The law<br />

of motion of the po<strong>in</strong>t M, is x = acoscof; the velocity<br />

at time / is<br />

aws<strong>in</strong>cof; the acceleration at time / is acD 2 cos(of. Initial velocity, 0;<br />

<strong>in</strong>itial acceleration: aw2 ; velocity when * = is -aco; acceleration when<br />

* = is 0. The maximum absolute value of velocity is aa>; the maximum<br />

absolute value of acceleration is aw2 . 687. y (n) = n\a n . 688. a) n\ (n+l<br />

(1 x)~ \<br />

b) ( _ ir + i ~<br />

. 689 .

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