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

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Hence, on the basis of formulas (1) and (2), we get<br />

and<br />

1<br />

R ~( fl i + 6i)<br />

JDL VaT+b*^ a<br />

a<br />

/. "fl' + a 1<br />

1 a*b = b<br />

~ 2<br />

a<br />

Q<br />

(a 2 + b*)~~ a 2 '<br />

2 + b<br />

Thus, for a screw-l<strong>in</strong>e, the curvature and torsion are constants.<br />

3 Fre<strong>net</strong> formulas:<br />

dr _ v ^v ___ T iP ^P_ v<br />

7s~"~R '<br />

5s ~~<br />

'<br />

~~~~R~T~~Q ds~~~~o"'<br />

2104. Prove that if the curvature at all po<strong>in</strong>ts of a l<strong>in</strong>e is<br />

zero, then the l<strong>in</strong>e is a straight l<strong>in</strong>e.<br />

2105. Prove that if the torsion at all po<strong>in</strong>ts of a curve is zero,<br />

then the<br />

2106.<br />

curve is a<br />

Prove that<br />

plane curve.<br />

the curve<br />

x=\+3t + 2t 2<br />

, y = 22t + 5t\ z=lt*<br />

is a plane curve; f<strong>in</strong>d the plane <strong>in</strong> which it lies.<br />

2107. Compute the curvature of the follow<strong>in</strong>g curves:<br />

a) x = cost, y = s'mt, z = cosh / at the / po<strong>in</strong>t = 0;<br />

b) x* 2<br />

// -| z 2 2 = l, y -2x + z = Q at the po<strong>in</strong>t (1, 1, 1).<br />

2108. Compute the curvature and torsion at curves:<br />

any po<strong>in</strong>t of the<br />

a) je = e'cos/, y = e i<br />

s<strong>in</strong>t, z e*\<br />

b) x^acosht, y asiuht. z = at (hyperbolic screw-l<strong>in</strong>e).<br />

2109. F<strong>in</strong>d the radii of curvature and torsion at an arbitrary<br />

po<strong>in</strong>t (x, y, z) of the curves:<br />

a) x 2 =<br />

b) x 9 =<br />

2110. Prove that the tangential and normal components of<br />

acceleration w are expressed by the formulas<br />

dv v 2<br />

VOif T

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