ANSWER on Question #70833 – Math – Geometry
QUESTION
Which of the following curves are regular?
1)
γ ( t ) = ( cos 2 t , sin 2 t ) , for − ∞ < t < ∞ \gamma(t) = (\cos^2 t, \sin^2 t), \quad \text{for} \quad -\infty < t < \infty γ ( t ) = ( cos 2 t , sin 2 t ) , for − ∞ < t < ∞
2)
γ ( t ) = ( cos 2 t , sin 2 t ) , for 0 < t < π 2 \gamma(t) = (\cos^2 t, \sin^2 t), \quad \text{for} \quad 0 < t < \frac{\pi}{2} γ ( t ) = ( cos 2 t , sin 2 t ) , for 0 < t < 2 π
3)
γ ( t ) = ( t , cosh t ) , for − ∞ < t < ∞ \gamma(t) = (t, \cosh t), \quad \text{for} \quad -\infty < t < \infty γ ( t ) = ( t , cosh t ) , for − ∞ < t < ∞
Find unit speed reparametrisation of regular curve(s).
SOLUTION
By the definition, let γ ( t ) \gamma(t) γ ( t ) be a curve. The velocity vector of γ ( t ) \gamma(t) γ ( t ) at t t t is γ ′ ( t ) \gamma'(t) γ ′ ( t ) .
The speed at t t t is a length ∣ γ ′ ( t ) ∣ |\gamma'(t)| ∣ γ ′ ( t ) ∣ .
γ ( t ) = ( x ( t ) , y ( t ) , z ( t ) ) → γ ′ ( t ) = ( x ′ ( t ) , y ′ ( t ) , z ′ ( t ) ) \gamma(t) = (x(t), y(t), z(t)) \rightarrow \gamma'(t) = (x'(t), y'(t), z'(t)) γ ( t ) = ( x ( t ) , y ( t ) , z ( t )) → γ ′ ( t ) = ( x ′ ( t ) , y ′ ( t ) , z ′ ( t )) ∣ γ ′ ( t ) ∣ = ( x ′ ( t ) ) 2 + ( y ′ ( t ) ) 2 + ( z ′ ( t ) ) 2 |\gamma'(t)| = \sqrt{(x'(t))^2 + (y'(t))^2 + (z'(t))^2} ∣ γ ′ ( t ) ∣ = ( x ′ ( t ) ) 2 + ( y ′ ( t ) ) 2 + ( z ′ ( t ) ) 2
By the definition, the curve γ ( t ) \gamma(t) γ ( t ) is regular if all velocity vectors are different from zero, that is,
γ ′ ( t ) ≠ 0 , ∀ t \gamma'(t) \neq 0, \forall t γ ′ ( t ) = 0 , ∀ t
In our case,
1)
γ ( t ) = ( cos 2 t , sin 2 t ) , for − ∞ < t < ∞ \gamma(t) = (\cos^2 t, \sin^2 t), \quad \text{for} \quad -\infty < t < \infty γ ( t ) = ( cos 2 t , sin 2 t ) , for − ∞ < t < ∞ x ( t ) = cos 2 t → x ′ ( t ) = 2 ⋅ ( cos t ) ⋅ ( − sin t ) = − sin ( 2 t ) ↔ x ′ ( t ) = − sin ( 2 t ) x(t) = \cos^2 t \rightarrow x'(t) = 2 \cdot (\cos t) \cdot (-\sin t) = -\sin(2t) \leftrightarrow \boxed{x'(t) = -\sin(2t)} x ( t ) = cos 2 t → x ′ ( t ) = 2 ⋅ ( cos t ) ⋅ ( − sin t ) = − sin ( 2 t ) ↔ x ′ ( t ) = − sin ( 2 t ) y ( t ) = sin 2 t → y ′ ( t ) = 2 ⋅ ( sin t ) ⋅ ( cos t ) = sin ( 2 t ) ↔ y ′ ( t ) = sin ( 2 t ) y(t) = \sin^2 t \rightarrow y'(t) = 2 \cdot (\sin t) \cdot (\cos t) = \sin(2t) \leftrightarrow \boxed{y'(t) = \sin(2t)} y ( t ) = sin 2 t → y ′ ( t ) = 2 ⋅ ( sin t ) ⋅ ( cos t ) = sin ( 2 t ) ↔ y ′ ( t ) = sin ( 2 t )
Then,
γ ′ ( t ) = ( − sin ( 2 t ) , sin ( 2 t ) ) \gamma'(t) = (-\sin(2t), \sin(2t)) γ ′ ( t ) = ( − sin ( 2 t ) , sin ( 2 t )) γ ′ ( π k ) = ( − sin ( 2 ⋅ ( π k ) ) , sin ( 2 ⋅ ( π k ) ) ) = ( 0 , 0 ) \gamma'(\pi k) = \left(-\sin\left(2 \cdot (\pi k)\right), \sin\left(2 \cdot (\pi k)\right)\right) = (0, 0) γ ′ ( πk ) = ( − sin ( 2 ⋅ ( πk ) ) , sin ( 2 ⋅ ( πk ) ) ) = ( 0 , 0 )
Conclusion,
γ ′ ( t ) = 0 , ∀ t = π k , k ∈ Z → \gamma'(t) = 0, \forall t = \pi k, k \in \mathbb{Z} \rightarrow γ ′ ( t ) = 0 , ∀ t = πk , k ∈ Z → γ ( t ) = ( cos 2 t , sin 2 t ) , for − ∞ < t < ∞ isn’t regular \gamma(t) = (\cos^2 t, \sin^2 t), \quad \text{for } -\infty < t < \infty \text{ isn't regular} γ ( t ) = ( cos 2 t , sin 2 t ) , for − ∞ < t < ∞ isn’t regular
2)
γ ( t ) = ( cos 2 t , sin 2 t ) , for 0 < t < π 2 \gamma(t) = (\cos^2 t, \sin^2 t), \quad \text{for } 0 < t < \frac{\pi}{2} γ ( t ) = ( cos 2 t , sin 2 t ) , for 0 < t < 2 π x ( t ) = cos 2 t → x ′ ( t ) = 2 ⋅ ( cos t ) ⋅ ( − sin t ) = − sin ( 2 t ) ↔ x ′ ( t ) = − sin ( 2 t ) x(t) = \cos^2 t \rightarrow x'(t) = 2 \cdot (\cos t) \cdot (-\sin t) = -\sin(2t) \leftrightarrow x'(t) = -\sin(2t) x ( t ) = cos 2 t → x ′ ( t ) = 2 ⋅ ( cos t ) ⋅ ( − sin t ) = − sin ( 2 t ) ↔ x ′ ( t ) = − sin ( 2 t ) y ( t ) = sin 2 t → y ′ ( t ) = 2 ⋅ ( sin t ) ⋅ ( cos t ) = sin ( 2 t ) ↔ y ′ ( t ) = sin ( 2 t ) y(t) = \sin^2 t \rightarrow y'(t) = 2 \cdot (\sin t) \cdot (\cos t) = \sin(2t) \leftrightarrow y'(t) = \sin(2t) y ( t ) = sin 2 t → y ′ ( t ) = 2 ⋅ ( sin t ) ⋅ ( cos t ) = sin ( 2 t ) ↔ y ′ ( t ) = sin ( 2 t )
Since the
0 < t < π 2 → 0 < ( 2 t ) < π 0 < t < \frac{\pi}{2} \rightarrow 0 < (2t) < \pi 0 < t < 2 π → 0 < ( 2 t ) < π
As we know
sin ( 2 t ) ≠ 0 , ∀ 0 < t < π 2 \sin(2t) \neq 0, \forall 0 < t < \frac{\pi}{2} sin ( 2 t ) = 0 , ∀0 < t < 2 π
Then,
γ ′ ( t ) = ( − sin ( 2 t ) , sin ( 2 t ) ) → γ ′ ( t ) ≠ 0 , ∀ 0 < t < π 2 \gamma'(t) = (-\sin(2t), \sin(2t)) \rightarrow \gamma'(t) \neq 0, \forall 0 < t < \frac{\pi}{2} γ ′ ( t ) = ( − sin ( 2 t ) , sin ( 2 t )) → γ ′ ( t ) = 0 , ∀0 < t < 2 π
Conclusion,
γ ′ ( t ) ≠ 0 , ∀ 0 < t < π 2 → \gamma'(t) \neq 0, \forall 0 < t < \frac{\pi}{2} \rightarrow γ ′ ( t ) = 0 , ∀0 < t < 2 π → γ ( t ) = ( cos 2 t , sin 2 t ) , for 0 < t < π 2 is regular \gamma(t) = (\cos^2 t, \sin^2 t), \quad \text{for } 0 < t < \frac{\pi}{2} \text{ is regular} γ ( t ) = ( cos 2 t , sin 2 t ) , for 0 < t < 2 π is regular
Now, we find the unit speed reparametrisation of regular curve γ ( t ) \gamma(t) γ ( t ) :
c = ∫ 0 π 2 ∣ γ ′ ( t ) ∣ d t = ∫ 0 π 2 ( − sin ( 2 t ) ) 2 + ( sin ( 2 t ) ) 2 d t = ∫ 0 π 2 2 ⋅ sin ( 2 t ) d t = 2 2 ⋅ ( − cos ( 2 t ) ) ∣ 0 π 2 = − 2 2 ⋅ ( cos ( 2 ⋅ π 2 ) − cos ( 2 ⋅ 0 ) ) = − 2 2 ⋅ ( cos ( π ) − cos ( 0 ) ) = = − 2 2 ⋅ ( − 1 − 1 ) = − 2 2 ⋅ ( − 2 ) = 2 → c = 2 \begin{array}{l} c = \int_ {0} ^ {\frac {\pi}{2}} | \gamma^ {\prime} (t) | d t = \int_ {0} ^ {\frac {\pi}{2}} \sqrt {(- \sin (2 t)) ^ {2} + (\sin (2 t)) ^ {2}} d t = \int_ {0} ^ {\frac {\pi}{2}} \sqrt {2} \cdot \sin (2 t) d t \\ = \frac {\sqrt {2}}{2} \cdot (- \cos (2 t)) \Bigg | _ {0} ^ {\frac {\pi}{2}} = - \frac {\sqrt {2}}{2} \cdot \left(\cos \left(2 \cdot \frac {\pi}{2}\right) - \cos (2 \cdot 0)\right) = - \frac {\sqrt {2}}{2} \cdot (\cos (\pi) - \cos (0)) = \\ = - \frac {\sqrt {2}}{2} \cdot (- 1 - 1) = - \frac {\sqrt {2}}{2} \cdot (- 2) = \sqrt {2} \rightarrow \boxed {c = \sqrt {2}} \\ \end{array} c = ∫ 0 2 π ∣ γ ′ ( t ) ∣ d t = ∫ 0 2 π ( − sin ( 2 t ) ) 2 + ( sin ( 2 t ) ) 2 d t = ∫ 0 2 π 2 ⋅ sin ( 2 t ) d t = 2 2 ⋅ ( − cos ( 2 t )) ∣ ∣ 0 2 π = − 2 2 ⋅ ( cos ( 2 ⋅ 2 π ) − cos ( 2 ⋅ 0 ) ) = − 2 2 ⋅ ( cos ( π ) − cos ( 0 )) = = − 2 2 ⋅ ( − 1 − 1 ) = − 2 2 ⋅ ( − 2 ) = 2 → c = 2
Then
s ( t ) = ∫ 0 t c d u = ∫ 0 t 2 d u = 2 t → t = s 2 s (t) = \int_ {0} ^ {t} c d u = \int_ {0} ^ {t} \sqrt {2} d u = \sqrt {2} t \rightarrow \boxed {t = \frac {s}{\sqrt {2}}} s ( t ) = ∫ 0 t c d u = ∫ 0 t 2 d u = 2 t → t = 2 s
Conclusion,
γ ( s ) = γ ( t ( s ) ) = ( cos 2 ( s 2 ) , sin 2 ( s 2 ) ) \boxed{\gamma(s) = \gamma(t(s)) = \left( \cos^2 \left( \frac{s}{\sqrt{2}} \right), \sin^2 \left( \frac{s}{\sqrt{2}} \right) \right)} γ ( s ) = γ ( t ( s )) = ( cos 2 ( 2 s ) , sin 2 ( 2 s ) ) is the unit speed reparametrisation
3)
γ ( t ) = ( t , cosh t ) , f o r − ∞ < t < ∞ \gamma (t) = (t, \cosh t), \quad f o r - \infty < t < \infty γ ( t ) = ( t , cosh t ) , f or − ∞ < t < ∞ x ( t ) = t → x ′ ( t ) = 1 ↔ x ′ ( t ) = 1 x (t) = t \rightarrow x ^ {\prime} (t) = 1 \leftrightarrow \boxed {x ^ {\prime} (t) = 1} x ( t ) = t → x ′ ( t ) = 1 ↔ x ′ ( t ) = 1 y ( t ) = cosh t → y ′ ( t ) = sinh t ↔ y ′ ( t ) = sinh t y (t) = \cosh t \rightarrow y ^ {\prime} (t) = \sinh t \leftrightarrow \boxed {y ^ {\prime} (t) = \sinh t} y ( t ) = cosh t → y ′ ( t ) = sinh t ↔ y ′ ( t ) = sinh t
Then,
γ ′ ( t ) = ( 1 , sinh t ) \gamma^ {\prime} (t) = (1, \sinh t) γ ′ ( t ) = ( 1 , sinh t )
Since the
1 ≠ 0 , 1 \neq 0, 1 = 0 ,
then
γ ′ ( t ) = ( 1 , sinh t ) ≠ 0 , f o r − ∞ < t < ∞ → \gamma^ {\prime} (t) = (1, \sinh t) \neq 0, f o r - \infty < t < \infty \rightarrow γ ′ ( t ) = ( 1 , sinh t ) = 0 , f or − ∞ < t < ∞ → γ ( t ) = ( t , cosh t ) , f o r − ∞ < t < ∞ is regular \boxed {\gamma (t) = (t, \cosh t), \quad f o r - \infty < t < \infty \text { is regular}} γ ( t ) = ( t , cosh t ) , f or − ∞ < t < ∞ is regular
Now, we find the unit speed reparametrisation of regular curve γ ( t ) \gamma(t) γ ( t )
s ( t ) = ∫ 0 t ∣ γ ′ ( u ) ∣ d u = ∫ 0 t 1 2 + ( sinh u ) 2 d u = [ As we know cosh 2 x − sinh 2 x = 1 cosh 2 x = 1 + sinh 2 x ] = = ∫ 0 t cosh 2 u d u = ∫ 0 t cosh u d u = sinh u ∣ 0 t = sinh t s(t) = \int_{0}^{t} |\gamma'(u)| \, du = \int_{0}^{t} \sqrt{1^2 + (\sinh u)^2} \, du = \begin{bmatrix} \text{As we know} \\ \cosh^2 x - \sinh^2 x = 1 \\ \cosh^2 x = 1 + \sinh^2 x \end{bmatrix} = \\
= \int_{0}^{t} \sqrt{\cosh^2 u} \, du = \int_{0}^{t} \cosh u \, du = \sinh u|_0^t = \sinh t s ( t ) = ∫ 0 t ∣ γ ′ ( u ) ∣ d u = ∫ 0 t 1 2 + ( sinh u ) 2 d u = ⎣ ⎡ As we know cosh 2 x − sinh 2 x = 1 cosh 2 x = 1 + sinh 2 x ⎦ ⎤ = = ∫ 0 t cosh 2 u d u = ∫ 0 t cosh u d u = sinh u ∣ 0 t = sinh t s ( t ) = sinh t → t ( s ) = asinh s s(t) = \sinh t \rightarrow \boxed{t(s) = \operatorname{asinh}s} s ( t ) = sinh t → t ( s ) = asinh s
Conclusion,
γ ( s ) = γ ( t ( s ) ) = ( asinh s , cosh ( asinh s ) ) − the unit speed reparametrisation \boxed{\gamma(s) = \gamma(t(s)) = (\operatorname{asinh}s, \cosh(\operatorname{asinh}s)) - \text{the unit speed reparametrisation}} γ ( s ) = γ ( t ( s )) = ( asinh s , cosh ( asinh s )) − the unit speed reparametrisation ANSWER:
1)
γ ( t ) = ( cos 2 t , sin 2 t ) for − ∞ < t < ∞ \gamma(t) = (\cos^2 t, \sin^2 t) \quad \text{for} \quad -\infty < t < \infty γ ( t ) = ( cos 2 t , sin 2 t ) for − ∞ < t < ∞ isn’t regular \text{isn't regular} isn’t regular
2)
γ ( t ) = ( cos 2 t , sin 2 t ) , for 0 < t < π 2 \gamma(t) = (\cos^2 t, \sin^2 t), \quad \text{for} \quad 0 < t < \frac{\pi}{2} γ ( t ) = ( cos 2 t , sin 2 t ) , for 0 < t < 2 π is regular \text{is regular} is regular γ ( s ) = ( cos 2 ( s 2 ) , sin 2 ( s 2 ) ) is the unit speed reparametrisation \boxed{\gamma(s)} = \left(\cos^2 \left(\frac{s}{\sqrt{2}}\right), \sin^2 \left(\frac{s}{\sqrt{2}}\right)\right) \text{ is the unit speed reparametrisation} γ ( s ) = ( cos 2 ( 2 s ) , sin 2 ( 2 s ) ) is the unit speed reparametrisation
3)
γ ( t ) = ( t , cosh t ) for − ∞ < t < ∞ \gamma(t) = (t, \cosh t) \quad \text{for} \quad -\infty < t < \infty γ ( t ) = ( t , cosh t ) for − ∞ < t < ∞ is regular \text{is regular} is regular γ ( s ) = ( asinh s , cosh ( asinh s ) ) is the unit speed reparametrisation \boxed{\gamma(s)} = (\operatorname{asinh}s, \cosh(\operatorname{asinh}s)) \text{ is the unit speed reparametrisation} γ ( s ) = ( asinh s , cosh ( asinh s )) is the unit speed reparametrisation
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