Question on $B$ unit vector in frenet frame
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Given a regular curve $a(s) in mathbb{R}^3$, we can attach a moving frame given by three orthogonal unit vectors, $T(s), N(s), B(s)$.
Now, my question is does $B'(s)$ (the derivative of the $B(s)$ unit vector, which we obtained from taking $T(s) times N(s)$ only depend on the it's projection with respect to $N(s)$?
That is to say, $B'(s)= tau N$, where $tau$ is the torsion of the curve. I follow my books argument, and it seems to be technical rather than intuitive. To me, it seems like the rate of change of $B(s)$ should also depend on it's projection against $T$ also. It'd be possible for the rotation of the $B(s)$ vector to be completely in the $BT$ plane (the rectifying plane?), and if this is true, $B'(s) neq 0$ but none of this change in position of $B(s)$ that it's derative represents will be in the direction of the $N$ vector. Am I making myself clear on why I'm confused?
differential-geometry
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add a comment |
$begingroup$
Given a regular curve $a(s) in mathbb{R}^3$, we can attach a moving frame given by three orthogonal unit vectors, $T(s), N(s), B(s)$.
Now, my question is does $B'(s)$ (the derivative of the $B(s)$ unit vector, which we obtained from taking $T(s) times N(s)$ only depend on the it's projection with respect to $N(s)$?
That is to say, $B'(s)= tau N$, where $tau$ is the torsion of the curve. I follow my books argument, and it seems to be technical rather than intuitive. To me, it seems like the rate of change of $B(s)$ should also depend on it's projection against $T$ also. It'd be possible for the rotation of the $B(s)$ vector to be completely in the $BT$ plane (the rectifying plane?), and if this is true, $B'(s) neq 0$ but none of this change in position of $B(s)$ that it's derative represents will be in the direction of the $N$ vector. Am I making myself clear on why I'm confused?
differential-geometry
$endgroup$
add a comment |
$begingroup$
Given a regular curve $a(s) in mathbb{R}^3$, we can attach a moving frame given by three orthogonal unit vectors, $T(s), N(s), B(s)$.
Now, my question is does $B'(s)$ (the derivative of the $B(s)$ unit vector, which we obtained from taking $T(s) times N(s)$ only depend on the it's projection with respect to $N(s)$?
That is to say, $B'(s)= tau N$, where $tau$ is the torsion of the curve. I follow my books argument, and it seems to be technical rather than intuitive. To me, it seems like the rate of change of $B(s)$ should also depend on it's projection against $T$ also. It'd be possible for the rotation of the $B(s)$ vector to be completely in the $BT$ plane (the rectifying plane?), and if this is true, $B'(s) neq 0$ but none of this change in position of $B(s)$ that it's derative represents will be in the direction of the $N$ vector. Am I making myself clear on why I'm confused?
differential-geometry
$endgroup$
Given a regular curve $a(s) in mathbb{R}^3$, we can attach a moving frame given by three orthogonal unit vectors, $T(s), N(s), B(s)$.
Now, my question is does $B'(s)$ (the derivative of the $B(s)$ unit vector, which we obtained from taking $T(s) times N(s)$ only depend on the it's projection with respect to $N(s)$?
That is to say, $B'(s)= tau N$, where $tau$ is the torsion of the curve. I follow my books argument, and it seems to be technical rather than intuitive. To me, it seems like the rate of change of $B(s)$ should also depend on it's projection against $T$ also. It'd be possible for the rotation of the $B(s)$ vector to be completely in the $BT$ plane (the rectifying plane?), and if this is true, $B'(s) neq 0$ but none of this change in position of $B(s)$ that it's derative represents will be in the direction of the $N$ vector. Am I making myself clear on why I'm confused?
differential-geometry
differential-geometry
asked Jan 23 at 2:57


Math is hardMath is hard
822211
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In order for two unit vectors to stay perpendicular, the second must turn away from the first at precisely the same rate as the first turns toward the second. (Mathematically, this is saying $B'cdot T = -T'cdot B$.) You can prove this by the product rule, but it's also quite clear if you just rotate your hand, keeping the thumb and forefinger perpendicular.
Since by definition $T$ turns only toward $N$ (i.e., it rotates in the osculating plane, instantaneously), it doesn't turn at all toward $B$ and so $B$ can't turn at all toward $T$.
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$begingroup$
Thanks for the response, i'm honored!
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– Math is hard
Jan 24 at 2:43
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$begingroup$
In order for two unit vectors to stay perpendicular, the second must turn away from the first at precisely the same rate as the first turns toward the second. (Mathematically, this is saying $B'cdot T = -T'cdot B$.) You can prove this by the product rule, but it's also quite clear if you just rotate your hand, keeping the thumb and forefinger perpendicular.
Since by definition $T$ turns only toward $N$ (i.e., it rotates in the osculating plane, instantaneously), it doesn't turn at all toward $B$ and so $B$ can't turn at all toward $T$.
$endgroup$
$begingroup$
Thanks for the response, i'm honored!
$endgroup$
– Math is hard
Jan 24 at 2:43
add a comment |
$begingroup$
In order for two unit vectors to stay perpendicular, the second must turn away from the first at precisely the same rate as the first turns toward the second. (Mathematically, this is saying $B'cdot T = -T'cdot B$.) You can prove this by the product rule, but it's also quite clear if you just rotate your hand, keeping the thumb and forefinger perpendicular.
Since by definition $T$ turns only toward $N$ (i.e., it rotates in the osculating plane, instantaneously), it doesn't turn at all toward $B$ and so $B$ can't turn at all toward $T$.
$endgroup$
$begingroup$
Thanks for the response, i'm honored!
$endgroup$
– Math is hard
Jan 24 at 2:43
add a comment |
$begingroup$
In order for two unit vectors to stay perpendicular, the second must turn away from the first at precisely the same rate as the first turns toward the second. (Mathematically, this is saying $B'cdot T = -T'cdot B$.) You can prove this by the product rule, but it's also quite clear if you just rotate your hand, keeping the thumb and forefinger perpendicular.
Since by definition $T$ turns only toward $N$ (i.e., it rotates in the osculating plane, instantaneously), it doesn't turn at all toward $B$ and so $B$ can't turn at all toward $T$.
$endgroup$
In order for two unit vectors to stay perpendicular, the second must turn away from the first at precisely the same rate as the first turns toward the second. (Mathematically, this is saying $B'cdot T = -T'cdot B$.) You can prove this by the product rule, but it's also quite clear if you just rotate your hand, keeping the thumb and forefinger perpendicular.
Since by definition $T$ turns only toward $N$ (i.e., it rotates in the osculating plane, instantaneously), it doesn't turn at all toward $B$ and so $B$ can't turn at all toward $T$.
answered Jan 23 at 21:00


Ted ShifrinTed Shifrin
64.2k44692
64.2k44692
$begingroup$
Thanks for the response, i'm honored!
$endgroup$
– Math is hard
Jan 24 at 2:43
add a comment |
$begingroup$
Thanks for the response, i'm honored!
$endgroup$
– Math is hard
Jan 24 at 2:43
$begingroup$
Thanks for the response, i'm honored!
$endgroup$
– Math is hard
Jan 24 at 2:43
$begingroup$
Thanks for the response, i'm honored!
$endgroup$
– Math is hard
Jan 24 at 2:43
add a comment |
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