6. The formula for the x -values is a little harder. The most helpful points from the table are ( 1 , 1 ) , ( 1 , 3 ) , ( 3 , 1 ) . (Hint: Consider inverse trigonometric functions.)
6. The formula for the x -values is a little harder. The most helpful points from the table are ( 1 , 1 ) , ( 1 , 3 ) , ( 3 , 1 ) . (Hint: Consider inverse trigonometric functions.)
6. The formula for the x-values is a little harder. The most helpful points from the table are
(
1
,
1
)
,
(
1
,
3
)
,
(
3
,
1
)
. (Hint: Consider inverse trigonometric functions.)
Show that the Laplace equation in Cartesian coordinates:
J²u
J²u
+
= 0
მx2 Jy2
can be reduced to the following form in cylindrical polar coordinates:
湯(
ди
1 8²u
+
Or 7,2 მ)2
= 0.
Draw the following graph on the interval
πT
5π
< x <
x≤
2
2
y = 2 cos(3(x-77)) +3
6+
5
4-
3
2
1
/2 -π/3 -π/6
Clear All Draw:
/6 π/3 π/2 2/3 5/6 x 7/6 4/3 3/2 5/311/6 2 13/67/3 5
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Determine the moment about the origin O of the force F4i-3j+5k that acts at a Point A. Assume that the position vector of A is (a) r =2i+3j-4k, (b) r=-8i+6j-10k, (c) r=8i-6j+5k
Probability And Statistical Inference (10th Edition)
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Fundamental Trigonometric Identities: Reciprocal, Quotient, and Pythagorean Identities; Author: Mathispower4u;https://www.youtube.com/watch?v=OmJ5fxyXrfg;License: Standard YouTube License, CC-BY