| 1 | ||
f(x0)= | ||
| cos2x0 |
| 1 | π | π | |||
=4, dla x∊(− | , | ) | |||
| cos2x0 | 2 | 2 |
| 1 | ||
cos2x0= | ||
| 4 |
| 1 | ||
|cosx0|= | , czyli | |
| 2 |
| π | π | |||
x0= | lub x0=− | |||
| 3 | 3 |
| π | −π | |||
y0=tg | =√3 y0=tg | =−√3 | ||
| 3 | 3 |
| π | π | |||
y−√3=4(x− | ) lub y+√3=4(x+ | ) | ||
| 3 | 3 |
| 4π | 4π | |||
y=4x− | +√3 lub y=4x+ | −√3 | ||
| 3 | 3 |