Texas Instruments Voyage 200, Руководство пользователя

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Appendix A: Functions and Instructions 877
sin
ê
(
squareMatrix1
)
⇒
⇒ ⇒
⇒
squareMatrix
Returns the matrix inverse sine of squareMatrix1 .
This is
not
the same as calculating the inverse
sine of each element. For information about the
calculation method, refer to
cos()
.
squareMatrix1 must be diagonalizable. The result
always contains floating-point numbers.
In Radian angle mode and Rectangular complex
format mode:
sin
ê
([1,5,3;4,2,1;6,
ë
2,1])
¸
sinh()
MATH/Hyperbolic menu
sinh( expression1 )
⇒ ⇒ ⇒ ⇒
expression
sinh( list1 )
⇒ ⇒ ⇒ ⇒
list
sinh (
expression1
)
returns the hyperbolic sine of
the argument as an expression.
sinh (
list
)
returns a list of the hyperbolic sines of
each element of list1 .
sinh(1.2)
¸
1.509
...
sinh({0,1.2,3.})
¸
{0 1.509
...
10.017
...
}
sinh(
squareMatrix1
)
⇒ ⇒ ⇒ ⇒
squareMatrix
Returns the matrix hyperbolic sine of
squareMatrix1
. This is not the same as calculating
the hyperbolic sine of each element. For
information about the calculation method, refer
to
cos()
.
squareMatrix1
must be diagonalizable. The result
always contains floating-point numbers.
In Radian angle mode:
sinh([1,5,3;4,2,1;6,
ë
2,1])
¸






360.954 305.708 239.604
352.912 233.495 193.564
298.632 154.599 140.251
sinh
ê
()
MATH/Hyperbolic menu
sinh
ê
(
expression1
)
⇒
⇒ ⇒
⇒
expression
sinh
ê
(
list1
)
⇒
⇒ ⇒
⇒
list
sinh ê (
expression1
)
returns the inverse hyperbolic
sine of the argument as an expression.
sinh ê ( list1 )
returns a list of the inverse
hyperbolic sines of each element of
list1
.
sinh
ê
(0)
¸
0
sinh
ê
({0,2.1,3})
¸
{0 1.487
...
sinh
ê
(3)}
sinh
ê
(
squareMatrix1
)
⇒
⇒ ⇒
⇒
squareMatrix
Returns the matrix inverse hyperbolic sine of
squareMatrix1 . This is
not
the same as calculating
the inverse hyperbolic sine of each element. For
information about the calculation method, refer
to
cos()
.
squareMatrix1 must be diagonalizable. The result
always contains floating-point numbers.
In Radian angle mode:
sinh
ê
([1,5,3;4,2,1;6,
ë
2,1])
¸






.041… 2.155… 1.158…
1.463… .926… .112…
2.750…
ë
1.528… .572…