拋物線公式

y = ax^2+bx+c 就是y等于ax的平方加上b

a > 0時開口向上

a < 0時開口向下

c = 0時拋物線經(jīng)過原點

b = 0時拋物線對稱軸為y軸

拋物線標準方程:y^2=2px

它表示拋物線的焦點在x的正半軸上,焦點坐標為(p/2,0)準線方程為x=-p/2

由于拋物線的焦點可在任意半軸,故共有標準方程y^2=2px y^2=-2px x^2=2py x^2=-2py

三角函數(shù)公式

sin(2kπ+α)=sinα

cos(2kπ+α)=cosα

tan(2kπ+α)=tanα

cot(2kπ+α)=cotα

sin(π+α)=-sinα

cos(π+α)=-cosα

tan(π+α)=tanα

cot(π+α)=cotα

sin(-α)=-sinα

cos(-α)=cosα

tan(-α)=-tanα

cot(-α)=-cotα

sin(π-α)=sinα

cos(π-α)=-cosα

tan(π-α)=-tanα

cot(π-α)=-cotα

sin(2π-α)=-sinα

cos(2π-α)=cosα

tan(2π-α)=-tanα

cot(2π-α)=-cotα

sin(π/2+α)=cosα

cos(π/2+α)=-sinα

tan(π/2+α)=-cotα

cot(π/2+α)=-tanα

sin(π/2-α)=cosα

cos(π/2-α)=sinα

tan(π/2-α)=cotα

cot(π/2-α)=tanα

sin(3π/2+α)=-cosα

cos(3π/2+α)=sinα

tan(3π/2+α)=-cotα

cot(3π/2+α)=-tanα

sin(3π/2-α)=-cosα

cos(3π/2-α)=-sinα

tan(3π/2-α)=cotα

cot(3π/2-α)=tanα

(以上k∈Z)

sin(A+B)=sinAcosB+cosAsinB sin(A-B)=sinAcosB-sinBcosA

cos(A+B)=cosAcosB-sinAsinB cos(A-B)=cosAcosB+sinAsinB

tan(A+B)=(tanA+tanB)/(1-tanAtanB) tan(A-B)=(tanA-tanB)/(1+tanAtanB)

ctg(A+B)=(ctgActgB-1)/(ctgB+ctgA) ctg(A-B)=(ctgActgB+1)/(ctgB-ctgA)

倍角公式

tan2A=2tanA/(1-tan2A) ctg2A=(ctg2A-1)/2ctga

cos2a=cos2a-sin2a=2cos2a-1=1-2sin2a

半角公式

sin(A/2)=√((1-cosA)/2) sin(A/2)=-√((1-cosA)/2)

cos(A/2)=√((1+cosA)/2) cos(A/2)=-√((1+cosA)/2)

tan(A/2)=√((1-cosA)/((1+cosA)) tan(A/2)=-√((1-cosA)/((1+cosA))

ctg(A/2)=√((1+cosA)/((1-cosA)) ctg(A/2)=-√((1+cosA)/((1-cosA))

和差化積

2sinAcosB=sin(A+B)+sin(A-B) 2cosAsinB=sin(A+B)-sin(A-B)

2cosAcosB=cos(A+B)-sin(A-B) -2sinAsinB=cos(A+B)-cos(A-B)

sinA+sinB=2sin((A+B)/2)cos((A-B)/2 cosA+cosB=2cos((A+B)/2)sin((A-B)/2)

tanA+tanB=sin(A+B)/cosAcosB tanA-tanB=sin(A-B)/cosAcosB

ctgA+ctgBsin(A+B)/sinAsinB -ctgA+ctgBsin(A+B)/sinAsinB