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x->0
tanx = x +o(x)
ln[ 1+ (2/3)tanx ]=(2/3)x +o(x)
1+ (2/3)tanx ] =(2/3)x^2 +o(x^2)
e^【 =e^[ 2/3)x^2 +o(x^2)] = 1+ (2/3)x^2 +o(x^2)
e^【 1 =(2/3)x^2 +o(x^2)
1+(2/3)tanx]^x -1 =e^【 1 =(2/3)x^2 +o(x^2)
lim(x->0) [3+2tanx)^x -3^x ] / [ 3(sinx)^2 + x^3. cos(1/x) ]
lim(x->0) 3^x. / [ 3(sinx)^2 + x^3. cos(1/x) ]
lim(x->0) / [ 3(sinx)^2 + x^3. cos(1/x) ]
lim(x->0) (2/3)x^2/ [ 3(sinx)^2 + x^3. cos(1/x) ]
The numerator denominator is divided by x 2 at the same time
lim(x->0) (2/3)/ [ 3(sinx/x)^2 + x. cos(1/x) ]
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You can't take a part of the addition of the numerator and replace it with the equivalent infinitesimal first, if it's a factor, it's okay, it's not an addition, this is a common mistake to find the limit, and you must figure it out. This question is best sought with Lobida.
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<> this question is more convenient and easier to understand by using the power series of sinx.
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From the question condition, it can be seen that the left = lim(x 0)(sin2x x +b x)+a=2 3.
Whereas, lim(x 0)(sin2x x +b x) = lim(x 0)(sin2x+bx) x. It belongs to the "0 0" type, using the rule of Lopida, lim(x 0)(sin2x x +b x) = lim(x 0)(2cos2x+b) (3x).
In this case, when x 0 and the denominator is 0, there must be 2cos2x+b 0. Again, 2cos2x+b is a continuous function, b=-2. ∴a=2/3。
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f(x) (0->(sinx) 2) ln(1+t) dt e (2x 2)-2e (x 2) +1] sell; x ≠ 0 loose matter
a Brewing liquid; x=0
x->0
Denominator. e^(2x^2) =1 +2x^2 +(1/2)(2x^2)^2 +o(x^4)=1 +2x^2 +2x^4 +o(x^4)
2e (x 2) = 2 +2x 2 + x 4 + o(x 4) e (2x 2)-2e (x 2) +1 = x 4 + o(x 4) molecules. sinx)^2 = x^2 +o(x^2)(0->(sinx)^2) ln(1+t) dt∫(0->(sinx)^2) t dt
0->x^2) t dt
1/2)x^4
lim(x->0) ∫0->(sinx)^2) ln(1+t) dt / e^(2x^2)-2e^(x^2) +1]
lim(x->0) (1/2)x^4 / x^4a=1/2<>
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Flexible use of the law of Lopida, stupid slag equivalence band quietly infinitesimal difference cavity substitution.
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Use Taylor's formula to spread the pure jerk method at x=0 points.
sinx=x-1/3!*x^3+o(x^4)f(x)=f(0)+f'(0)*x+f''(0)/2!*x^2+o(x^3)
Then (sinx+xf(x)) x 3
x-1/3!*x^3+o(x^4)+f(0)*x+f'(0)*x^2+f''(0)/2!*x^3+o(x^4))/x^3
1+f(0))*x+f'(0)*x^2+(f''(0)/2!-1/3!)*x^3+o(x^4))/x^3
If the limit holds, and is equal to 1 2
Then it can only be.
1+f(0)=0
f'(0)=0
f''(0)/2!-1/3!=1/2
Hence f(0)=-1
f'(0)=0
f''(0)=(1/2+1/3!)*2!=1+1 3=4 3If you are satisfied, please choose the one [Satisfied]. Thank you ......If there is still something unclear, Hungry Bridge can ask [chase] for the age of pants.
In addition, after selecting [Satisfied] and other treatments, you can return the wealth value of the mortgage.
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x 2 is derived from the equivalent infinitesimal substitution.
e^x-1)~x tanx~x
sin 2x x 2+(cosx-1) x 2 is still the result of an equivalent infinitesimal substitution.
sinx/x->1 cosx-1~-x^2/2 cosx-1/x^2->-1/2
So add it up to 1-1 2
If you don't understand, you can hi me.
Also note the references below.
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Answer: Let y=(x+e x) (1 x), take the natural logarithm, have: lny=ln(x+e x) x
When calculating x tends to positive infinity, use Robida's rule to calculate the limit of lny (a denotes the sign that the limit approaches positive infinity when x approaches positive infinity).
a(lny)=a[(1+e^x)/(x+e^x)]/1=a[e^x/(1+e^x)]=a[e^x/e^x]=1
So: original limit = e
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Omit the limit symbol. The original form can be written as.
1+x+e^x-1)^
Since the limit of [x+e x-1] x is 2, the original limit is e 2
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X is ignored when it tends to be positive infinity.
e^x)^(1/x)=e
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Click to enlarge and then click to enlarge again.
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There is something wrong with this problem itself: the limit is 1, regardless of the value of c
Solution: Let 2l=20cm, l=10cm
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