From: yen, ka-in on

Eric Gisse wrote:
> Area is not a vector - area is a SCALAR. Area of a rectangle is defined
> as the magnitude of the two vectors that form the sides of the
> rectangle.
>
> Which, unsurprisingly, IS NOT A VECTOR.

Your parent will be proud of you, if you can solve the problem
BY YOURSELF. CAN you?

Home work for Eric Gisse:
A rectangle sits in 3D space. The area vector of the rectangle is A,
and the legth vector of one side of the rectangle is L. Please find
the length vector of the other side of the rectangle?

From: Eric Gisse on

yen, ka-in wrote:
> Eric Gisse wrote:
> > Area is not a vector - area is a SCALAR. Area of a rectangle is defined
> > as the magnitude of the two vectors that form the sides of the
> > rectangle.
> >
> > Which, unsurprisingly, IS NOT A VECTOR.
>
> Your parent will be proud of you, if you can solve the problem
> BY YOURSELF. CAN you?
>
> Home work for Eric Gisse:
> A rectangle sits in 3D space. The area vector of the rectangle is A,
> and the legth vector of one side of the rectangle is L. Please find
> the length vector of the other side of the rectangle?

Area is not a vector, retard.

From: Androcles on

"yen, ka-in" <yenkain(a)yahoo.com.tw> wrote in message
news:1162366326.610183.122090(a)e64g2000cwd.googlegroups.com...
|
| Eric Gisse wrote:
| > Area is not a vector - area is a SCALAR. Area of a rectangle is defined
| > as the magnitude of the two vectors that form the sides of the
| > rectangle.
| >
| > Which, unsurprisingly, IS NOT A VECTOR.
|
| Your parent will be proud of you, if you can solve the problem
| BY YOURSELF. CAN you?
|
| Home work for Eric Gisse:
| A rectangle sits in 3D space. The area vector of the rectangle is A,
| and the legth vector of one side of the rectangle is L. Please find
| the length vector of the other side of the rectangle?

Your question is ambiguous, a rectangle has 4 edges and 2 faces
for a total of 6 "sides".

Have the idiot explain how to open a door by pulling instead
of pushing.
Androcles


From: Ka-In Yen on
A major discovery at the beginning of 21st century -- the idiocy
of physicists. Stupid physicists have been doing vector by vector
division for a hundred years, but they are not aware it.

So stupid !!!


The proof of mass vector.

Ka-In Yen
http://www.geocities.com/redlorikee


Introduction:
In this paper, we will prove that linear mass density and
surface mass density are vector, and the application of mass
vector is presented.


1. The unit of vector.


In physics, The unit of three-dimensional cartesian coordinate
systems is meter. In this paper, a point of 3-D coordinate
system is written as


(p1,p2,p3) m, or (p:3) m


and a vector is written as


<a,b,c> m, or <a:3> m


or


l m<i,j,k> = <a,b,c> m


where l=abs(sqrt(a^2+b^2+c^2)) is the magnitude of the vector,
and <i,j,k> is a unit vector which gives the direction of
the vector.


For three reasons, a magnitude of a vector can not add to a
scalar:
i) The magnitude belongs to the set of vector; it's a
portion of a vector. Scalar belongs to a field.
ii) The magnitude is real non-negative number, but scalar
is real number.
iii) The unit of magnitude is meter, but scalar has no unit.
This is a major difference between physics and mathematics.
5m+3 is meaningless.


2. Linear mass density is a vector.


The mass of a string is M kg, and the length of the string
is l m<i:3>. Where l m is the magnitude of the length, and
<i:3> is a 3-D unit vector which gives the direction of the
string. Then the linear mass density of the string is:


M/(l<i:3>)=(M/l) (kg/m)<i:3>


The direction, <i:3>, is not changed by "division", so we
can move <i:3> from denominator to numerator. A direction
is changed by -1 only. A proof is found in Clifford algebras:


[Proof]
k/<a,b,c>=[k<a,b,c>]/[<a,b,c>^2]
=(k/l) <i,j,k>
where l is the magnitude of <a,b,c>, and <i,j,k> is the
unit vector of <a,b,c>.
[Proof]


3. Surface mass density is a vector.


A parallelogram has two vectors: l m<i:3> and h m<j:3>. <i:3>
and <j:3> are unit vectors. The area vector of the parallelogram
is the cross product of these two vectors.


l m<i:3> X h m<j:3>= lh (m^2 )<i:3>X<j:3>
= lh abs(sin(theta)) (m^2)<k:3>


Where theta is the angle between <i:3> and <j:3>. <k:3> is
a unit vector which is perpendicular to <i:3> and <j:3>.
For AXB=-BXA, an area has two directions.


We can divide the area vector by the length vector.


lh*abs(sin(theta))<k:3>/[l<i:3>]
=h<i:3>X<j:3>/<i:3>
=h(<i:3>X<j:3>)X<i:3>
(The direction, <i:3>, is not changed by "division", and
the division is replaced by a cross product.)
=-h<i:3>X(<i:3>X<j:3>)
=-h[<i:3>(<i:3>o<j:3>)-<j:3>(<i:3>o<i:3>)]
(where o is dot product.)
=-h(cos(theta)<i:3>-<j:3>)
=h(<j:3>-cos(theta)<i:3>) m


The result is a rectangle, not the original parallelogram. We
can test the result.


h(<j:3>-cos(theta)<i:3>)Xl<i:3>=lh m^2<j:3>X<i:3>


The magnitude of the area vector is conserved, but the direction
is opposite.


The mass of a round plate is M kg, and the area vector is
A m^2<i:3>; then the surface mass density is


M kg/(A m^2<i:3>)=M/A (kg/m^2)<i:3>


4. Mass vector in physics.


Mass vector has been found in two equations: 1) the velocity
equation of string. 2) Bernoulli's equation.


i) For waves on a string, we have the velocity equation:


v=sqrt(tau/mu). v is velocity of wave, tau is tension
applying to string, and mu is linear mass density of
string. We can rewrite the equation:


mu=tau/v^2.


In the above equation, the mu is parallel to tau, and both
of them are vector.


ii) Bernoulli's equation is:


P + k*v^2/2=C (P is pressure, k is volume density, and v is
velocity. Here we neglect the gravitational term.)


Multiplying cross area vector A m^2<i:3> of a string to Bernoulli's
equation(where <i:3> is a unit vector),


P*A<i:3> + k*A<i:3>*v^2/2=C*A<i:3>
F<i:3> + L<i:3>*v^2/2=C*A<i:3>
(where F is the magnitude of force, and L is the magnitude
of linear mass density.)


These two equations are well used in the theory "Magnetic force:
Combining Drag force and Bernoulli force of ether dynamics."
For detail, please refer to my site:
http://www.geocities.com/redlorikee

From: yen, ka-in on
In three dimensional vector algebra, area HAS TO be a vector,
and we can divide an area vector of a rectangle by the length
vector of this rectangle.



The proof of mass vector.

Ka-In Yen
http://www.geocities.com/redlorikee

Introduction:
In this paper, we will prove that linear mass density and
surface mass density are vector, and the application of mass
vector is presented.


1. The unit of vector.


In physics, The unit of three-dimensional cartesian coordinate
systems is meter. In this paper, a point of 3-D coordinate
system is written as


(p1,p2,p3) m, or (p:3) m


and a vector is written as


<a,b,c> m, or <a:3> m


or


l m<i,j,k> = <a,b,c> m


where l=abs(sqrt(a^2+b^2+c^2)) is the magnitude of the vector,
and <i,j,k> is a unit vector which gives the direction of
the vector.


For three reasons, a magnitude of a vector can not add to a
scalar:
i) The magnitude belongs to the set of vector; it's a
portion of a vector. Scalar belongs to a field.
ii) The magnitude is real non-negative number, but scalar
is real number.
iii) The unit of magnitude is meter, but scalar has no unit.
This is a major difference between physics and mathematics.
5m+3 is meaningless.


2. Linear mass density is a vector.


The mass of a string is M kg, and the length of the string
is l m<i:3>. Where l m is the magnitude of the length, and
<i:3> is a 3-D unit vector which gives the direction of the
string. Then the linear mass density of the string is:


M/(l<i:3>)=(M/l) (kg/m)<i:3>


The direction, <i:3>, is not changed by "division", so we
can move <i:3> from denominator to numerator. A direction
is changed by -1 only. A proof is found in Clifford algebras:


[Proof]
k/<a,b,c>=[k<a,b,c>]/[<a,b,c>^2]
=(k/l) <i,j,k>
where l is the magnitude of <a,b,c>, and <i,j,k> is the
unit vector of <a,b,c>.
[Proof]


3. Surface mass density is a vector.


A parallelogram has two vectors: l m<i:3> and h m<j:3>. <i:3>
and <j:3> are unit vectors. The area vector of the parallelogram
is the cross product of these two vectors.


l m<i:3> X h m<j:3>= lh (m^2 )<i:3>X<j:3>
= lh abs(sin(theta)) (m^2)<k:3>


Where theta is the angle between <i:3> and <j:3>. <k:3> is
a unit vector which is perpendicular to <i:3> and <j:3>.
For AXB=-BXA, an area has two directions.


We can divide the area vector by the length vector.


lh*abs(sin(theta))<k:3>/[l<i:3>]
=h<i:3>X<j:3>/<i:3>
=h(<i:3>X<j:3>)X<i:3>
(The direction, <i:3>, is not changed by "division", and
the division is replaced by a cross product.)
=-h<i:3>X(<i:3>X<j:3>)
=-h[<i:3>(<i:3>o<j:3>)-<j:3>(<i:3>o<i:3>)]
(where o is dot product.)
=-h(cos(theta)<i:3>-<j:3>)
=h(<j:3>-cos(theta)<i:3>) m


The result is a rectangle, not the original parallelogram. We
can test the result.


h(<j:3>-cos(theta)<i:3>)Xl<i:3>=lh m^2<j:3>X<i:3>


The magnitude of the area vector is conserved, but the direction
is opposite.


The mass of a round plate is M kg, and the area vector is
A m^2<i:3>; then the surface mass density is


M kg/(A m^2<i:3>)=M/A (kg/m^2)<i:3>


4. Mass vector in physics.


Mass vector has been found in two equations: 1) the velocity
equation of string. 2) Bernoulli's equation.


i) For waves on a string, we have the velocity equation:


v=sqrt(tau/mu). v is velocity of wave, tau is tension
applying to string, and mu is linear mass density of
string. We can rewrite the equation:


mu=tau/v^2.


In the above equation, the mu is parallel to tau, and both
of them are vector.


ii) Bernoulli's equation is:


P + k*v^2/2=C (P is pressure, k is volume density, and v is
velocity. Here we neglect the gravitational term.)


Multiplying cross area vector A m^2<i:3> of a string to Bernoulli's
equation(where <i:3> is a unit vector),


P*A<i:3> + k*A<i:3>*v^2/2=C*A<i:3>
F<i:3> + L<i:3>*v^2/2=C*A<i:3>
(where F is the magnitude of force, and L is the magnitude
of linear mass density.)


These two equations are well used in the theory "Magnetic force:
Combining Drag force and Bernoulli force of ether dynamics."
For detail, please refer to my site:
http://www.geocities.com/redlorikee

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