Question #99028

Because of a storm, ground controllers instruct the pilot of a plane flying at an altitude of 4 miles to make a turn and climb to an altitude of 4.2 miles. The model for the path of the plane during this maneuver is
r(t) = 10 cos 10π t i + 10 sin 10 π t j + ( 4+ 4t )k , 0≤ t≤ 1/20
where t is the time in hours and r is the position vector.
i. Determine the speed of the plane
ii. Calculate αT and αN

Expert's answer

Speed of the Plane


Given,

The model for the path of the plane during this maneuver is


r(t)=10cos10π i+10sin10πt j+(4+4t)k, 0t120r(t) = 10 cos 10\pi \space \vec i + 10 sin 10\pi t \space \vec j + (4 + 4t ) \vec k , \space 0\le t\le\frac {1}{20}

Here t is the time in hours and


r is the position vector


(a)


We can calculate the speed of the plane by the formula

r(t)||r' (t)||


So, Differentiate the position vector r(t) with respect to t



v(t)=r(t)=ddt(10cos10π i+10sin10πt j+(4+4t)k)v(t) = r' (t) = \frac {d}{dt} (10 cos 10\pi \space \vec i + 10 sin 10\pi t \space \vec j + (4 + 4t ) \vec k )

=100πsin10π t i + 100πcos10πt j+4k= - 100\pi sin 10\pi \space t \space \vec i \space + \space 100 \pi cos 10\pi t \space \vec j + 4 \vec k



Now the Speed of the plane =



v(t)=r(t)=100πsin10π t i + 100πcos10πt j+4k ||v(t) || = ||r' (t) || = || - 100 \pi sin 10\pi \space t \space \vec i \space + \space 100\pi cos 10\pi t \space \vec j + 4 \vec k \space ||


=(100πsin10πt)2+(100πcos10πt)2+42= \sqrt {(- 100 \pi sin10\pi t)^2 + (100\pi cos 10\pi t)^2 + 4^2 }=(10000π2sin210πt)+(10000π2cos210πt)+16= \sqrt {( 10000 \pi^2 sin^2 10\pi t) + (10000\pi^2 cos^2 10\pi t) + 16 }


=10000π2 [(sin2(10πt)+cos2(10πt)]+16= \sqrt {10000 \pi^2 \space [( sin^2 (10\pi t ) + cos^2 (10\pi t)] + 16}



v(t)=10000π2(1)+16=10000π2+16||v(t) || = \sqrt {10000\pi^2 (1) + 16} = \sqrt {10000\pi^2 + 16}

Now the Speed of the plane==4×625π2+1=314.025 miles/hrNow \space the \space Speed \space of \space the \space plane = = 4 \times \sqrt {625\pi^2 + 1} = 314.025 \space miles/hr

(b).


Now, we need to calculate the αT and αNα_{T} \space and \space α_{N}


Here, formula for Tangential acceleration is given by


αT=ddt[v]=v.αvα_{T} = \frac {d}{dt} [||v||] = \frac {v.α}{||v||}

We know,

α(t)=v(t)=ddt(100πsin10π t i + 100πcos10πt j+4k)α(t) = v'(t) = \frac {d}{dt} (- 100 \pi sin 10\pi \space t \space \vec i \space + \space 100 \pi cos 10\pi t \space \vec j + 4 \vec k )

=1000π2 cos10πti1000π2sin10πt j= -1000 \pi^2 \space cos 10\pi t \vec i - 1000 \pi^2 sin 10\pi t \space \vec j



v.α=(100πsin10π t i + 100πcos10πt j+4k).(1000π2 cos10πti1000π2sin10πt j)v.α = (- 100\pi sin 10\pi \space t \space \vec i \space + \space 100 \pi cos 10\pi t \space \vec j + 4 \vec k ). (-1000 \pi^2 \space cos 10\pi t \vec i - 1000 \pi^2 sin 10\pi t \space \vec j)


=100000π3sin(10πt) cos(10πt)100000π3sin(10πt)cos(10πt)+0= 100000\pi^3 sin (10\pi t) \space cos (10\pi t) - 100000 \pi^3 sin (10\pi t) cos (10\pi t) + 0


v.α=0v.α = 0


So, Tangential acceleration is

αT=v.αv=0314.025=0α_{T} = \frac {v.α}{||v||} = \frac {0} { 314.025} = 0

Here,  formula for Normal components of acceleration is given by


αN=v×αvα_{N} = \frac {||v \times α||}{||v||}


v×α=ijk100πsin(10πt)100πcos(10πt)41000π2cos(10πt)1000π2sin(10πt)0v \times α = \begin{vmatrix} i & j & k \\ -100 \pi sin (10\pi t) & 100\pi cos (10\pi t) & 4 \\ -1000\pi^2 cos (10\pi t) & -1000 \pi^2 sin (10\pi t) & 0 \end{vmatrix}


=i(0+4000π2sin(10πt))j(0+4000π2cos(10πt)+k(100000π3sin2(10πt+100000π3cos2(10πt))= i (0 + 4000 \pi^2 sin (10\pi t)) - j (0 + 4000\pi^2 cos (10\pi t) \\+ k ( 100000 \pi^3 sin^2 (10\pi t + 100000 \pi^3 cos^2 (10\pi t))

.


v×α==i(4000π2sin(10πt))j(4000π2cos(10πt)+k×100000π3(sin2(10πt+cos2(10πt)))v \times α = = i ( 4000 \pi^2 sin (10\pi t)) - j ( 4000\pi^2 cos (10\pi t) \\+ k \times 100000 \pi^3 (sin^2 (10\pi t + cos^2 (10\pi t)))


v×α=i(4000π2sin(10πt))j(4000π2cos(10πt)+k×100000π3v \times α = i ( 4000 \pi^2 sin (10\pi t)) - j ( 4000\pi^2 cos (10\pi t) \\+ k \times 100000 \pi^3


v×α=(4000π2)2sin2(10πt)+(4000π2)2cos2(10πt)+100002π6|| v \times α ||= \sqrt {(4000 \pi^2)^2 sin ^2(10\pi t) + (4000 \pi^2)^2 cos^2 (10\pi t) + 10000^2 \pi^6}

v×α=(4000π2)2 [sin2(10πt)+cos2(10πt)]+100002π6|| v \times α ||= \sqrt {(4000 \pi^2)^2 \space [sin ^2(10\pi t) + cos^2 (10\pi t)] + 10000^2 \pi^6}

v×α=(4000π2)2 +100002π6|| v \times α ||= \sqrt {(4000 \pi^2)^2 \space + 10000^2 \pi^6}



v×α=4000π21+625π2|| v \times α ||= 4000 \pi^2 \sqrt {1 +625 \pi^2}

αN=v×αv=4000π21+625π24×625π2+1α_{N} = \frac {||v \times α||}{||v||} = \frac {4000\pi^2 \sqrt {1+ 625\pi^2}}{4 \times \sqrt {625\pi^2 + 1}}

Normal components of acceleration is

αN=1000π2α_{N} = 1000 \pi^2



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