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How to proceed with streamlines
Vector field with bounded integral curvesFind the divergence of the following vector fieldsStokes theorem and the simple closed curve on which work is maximumConnect two points in $mathbb R^3$ using integral lines of some vector fieldsHow do I proceed towards the evaluation of this surface integral?In the context of curl, what does the difference between two partial derivatives tell me about rotation in a plane?Finding the derivative of a complicated vector to scalar functionCommutator of vector fields $x∂_x + y∂_y + z∂_z$ and $∂_z$Why is does this vector field have zero-curl everywhere? Plus, broad questions about curl.Considering the work done from two different paths
$begingroup$
I am starting with describing the streamlines of velocity fields.
Let's work out the following example so as to see where I get stuck:
$$v(x, y, z) = x hati + y hatj - x hatk$$
Now we set up the differential equation for the field lines:
$$fracdxx = fracdyy = - fracdzx$$
From here on I do not understand why we do what we do; the solution states:
Thus, $z + x = C_1$, $y = C_2 x$. The streamlines are straight halflines emanating from the z-axis
and perpendicular to the vector $hati + hatk$
Please explain why.
vector-analysis vector-fields
$endgroup$
add a comment |
$begingroup$
I am starting with describing the streamlines of velocity fields.
Let's work out the following example so as to see where I get stuck:
$$v(x, y, z) = x hati + y hatj - x hatk$$
Now we set up the differential equation for the field lines:
$$fracdxx = fracdyy = - fracdzx$$
From here on I do not understand why we do what we do; the solution states:
Thus, $z + x = C_1$, $y = C_2 x$. The streamlines are straight halflines emanating from the z-axis
and perpendicular to the vector $hati + hatk$
Please explain why.
vector-analysis vector-fields
$endgroup$
1
$begingroup$
$dfracdxx=-dfracdzximplies dx+dz=0implies x+z=C_1$. You can get the second equation by equating $dfracdxx$ and $dfracdyy$ and integrating in a similar manner.
$endgroup$
– Shubham Johri
Mar 13 at 19:02
add a comment |
$begingroup$
I am starting with describing the streamlines of velocity fields.
Let's work out the following example so as to see where I get stuck:
$$v(x, y, z) = x hati + y hatj - x hatk$$
Now we set up the differential equation for the field lines:
$$fracdxx = fracdyy = - fracdzx$$
From here on I do not understand why we do what we do; the solution states:
Thus, $z + x = C_1$, $y = C_2 x$. The streamlines are straight halflines emanating from the z-axis
and perpendicular to the vector $hati + hatk$
Please explain why.
vector-analysis vector-fields
$endgroup$
I am starting with describing the streamlines of velocity fields.
Let's work out the following example so as to see where I get stuck:
$$v(x, y, z) = x hati + y hatj - x hatk$$
Now we set up the differential equation for the field lines:
$$fracdxx = fracdyy = - fracdzx$$
From here on I do not understand why we do what we do; the solution states:
Thus, $z + x = C_1$, $y = C_2 x$. The streamlines are straight halflines emanating from the z-axis
and perpendicular to the vector $hati + hatk$
Please explain why.
vector-analysis vector-fields
vector-analysis vector-fields
asked Mar 13 at 18:57
JD_PMJD_PM
16111
16111
1
$begingroup$
$dfracdxx=-dfracdzximplies dx+dz=0implies x+z=C_1$. You can get the second equation by equating $dfracdxx$ and $dfracdyy$ and integrating in a similar manner.
$endgroup$
– Shubham Johri
Mar 13 at 19:02
add a comment |
1
$begingroup$
$dfracdxx=-dfracdzximplies dx+dz=0implies x+z=C_1$. You can get the second equation by equating $dfracdxx$ and $dfracdyy$ and integrating in a similar manner.
$endgroup$
– Shubham Johri
Mar 13 at 19:02
1
1
$begingroup$
$dfracdxx=-dfracdzximplies dx+dz=0implies x+z=C_1$. You can get the second equation by equating $dfracdxx$ and $dfracdyy$ and integrating in a similar manner.
$endgroup$
– Shubham Johri
Mar 13 at 19:02
$begingroup$
$dfracdxx=-dfracdzximplies dx+dz=0implies x+z=C_1$. You can get the second equation by equating $dfracdxx$ and $dfracdyy$ and integrating in a similar manner.
$endgroup$
– Shubham Johri
Mar 13 at 19:02
add a comment |
0
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1
$begingroup$
$dfracdxx=-dfracdzximplies dx+dz=0implies x+z=C_1$. You can get the second equation by equating $dfracdxx$ and $dfracdyy$ and integrating in a similar manner.
$endgroup$
– Shubham Johri
Mar 13 at 19:02