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Продовження таблиці 2.2
8 lg( 1 sin( m )) ln( 1 sin( n )) 3 83 0 2 16 0 4.6035 5.1546e-2
7 3
9 3 2 2 5 0.3 12 0 220 0 4.875e-1+ 7.3715e-1
sin ( m ) n sin ( m ) n
7 8.4448e-1i
10 log n ( ) 4 . 1 3 4 3.56 e 0.316 2 2.16410 -2 1.1790 1.6630
m
11 2 3 1 2 3 ln3 lg3 0.013 1.410 2 5.7737 6.6559e+1
m n m n
12 2 364.85 – 24 – 1.5880e+4 5.4516e-1
m m 3 m 4 m
3 37
13 8 m n e 1.11 7 5.403 28 0 2.8187 3.7879e-3
m sin 6
3 2 11
0
14 m n 1 5 ln7 1.34 -6.6313 5.0346e-6
2 tg ) n ( sin 2
2 . 0 03 7
15 1 m 3 cos( ) n -20.1 20 0 lg13.6 1.48 -3.0201e-2 8.5792e-3
12 (sin( ) n cos( n )) 3
16 3 0.28 41 0 e 0.415 237 0 8.1284e-2 4.9334
3 m
sin( n 30 ) sin( n 30 )
cos 2 ) n (
0 -2
17 n 2 6.178 20 -2.2410 1.146 3.5028e-2 1.4003
lg( m ) 2 tg ) n (
3
18 3 4 4 10.6 50 0 e 2.3 1 4.1645e+2 4.1101e+2
m ctg ) n ( sin ) n ( cos ) n (
19 m 2 3 5.08 25 0 ln1.37 12 1.6193e+3 3.5238e+3
4
(sec( ) n cos ec n ( ))
4 25
0 0
20 1 51 39 0.643 1.4132e-1 5.0772e-2
3 ( ctg ( m ) ctg n ( )) 2 7
21 2 8 e 1.648 – tg1.21 – 6.1109 -5.1927e-1
lg 3 m m 9
27
22 5 e 5 4 m ( m 12 . 36 ) 2 2.17510 2 – cos17 0 – 8.5511e+75 4.0272
ln( m ) 7
-1
23 27 m 1 e 2.145 – 2.46810 – -2.0936e+3 1.7858e-1
lg 2 m
8
24 1 e -0.37 ln2.1517 37 0 7 3.4445e-1 2.6745e-1
5 m( ) n 2 3 cos
n ( m ) 24
25 sin( m ) tg ) n ( 5.6 lg25 8 4.4466 5.2145e-1
5 2 9 10
( m 3 ) n