In[8]:=
D[y + 1, y] == D[x+Cos[y], x]
Out[8]=
True
b) Evaluate the integral of F . dx along C_1, where
where C_1 is the closed loop given by x(t) = cos(t),
y = t^2 - 2 9 t, 0 2 t 2 2 9.
Because the vector field is exact, the integral around any closed loop is 0,
It is not necessary to parametrize.
c) Evaluate the integral of F . dx,
where C_2 is the non-closed curve given by x(t) = cos(t), y = t^2 - 2 9 t, 0 2
t 2 9.
Because the vector field is exact, the vector field is the gradient of a scalar
function f[x,y], and the integral is just f[end point] - f[ starting point]. I
will
solve this by finding the scalar function f. Another valid possibility is to
use
the path-independence property, and do the integral directly along a straight
linefrom (1,0) to (-1,- pi^2).
To find x, integrate the components of the vector field and compare terms to
fix the "constants" of integration, by which I mean the arbitrary
functions of
one variable alone . I will write them explicitly:
In[9]:=
f[x, y] = Integrate[y + 1, x] + C1[y]
Out[9]=
x (1 + y) + C1[y]
In[10]:=
f[x, y] = Integrate[x + Cos[y], y] + C2[x]
Out[10]=
x y + C2[x] + Sin[y]
In[11]:=
% == %%
Out[11]=
x y + C2[x] + Sin[y] == x (1 + y) + C1[y]
Evidently, we can take C1[y] = Sin[y] and C2[x] = x, so
In[12]:=
Clear[f]
In[13]:=
f[x_,y_] = x y + x + Sin[y]
Out[13]=
x + x y + Sin[y]
Checking:
In[14]:=
{D[f[x,y], x], D[f[x,y], y]}
Out[14]=
{1 + y, x + Cos[y]}
The value of the integral is
In[15]:=
(%% /.{x -> -1, y -> - Pi^2}) - (%% /.{x -> 1, y -> 0})
Out[15]=
2 2 -2 + Pi - Sin[Pi ]
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