1.The remainder for a Taylor series is calculated as:
Rn(x)=(n+1)!f(n+1)(c)(x−a)(n+1) , where c is from the interval of approximation.
So the maximum error is calculated as:
∣Rn(x)∣≤(n+1)!M∣x−a∣(n+1) , where M is a maximum value of ∣f(n+1)(x)∣ on the interval.
In our case 5x5 is a fifth, so n=5. a=0. f(x)=sin(x), f'(x)=cos(x), f''(x)=-sin(x), f'''(x)=-cos(x), f''''(x)=sin(x).
f(5)(x)=cos(x),f(6)(x)=−sin(x) . sin is rising from -0.3 to 0.3 and sin(0.3)=-sin(-0.3), so M=sin(0.3) and we get the maximum error (where -0.3<x<0.3):
(n+1)!M∣x−a∣(n+1)=6!sin(0.3)∣x∣(6)≈0.00041∣x∣6 .
Let's calculate using this approximation:
sin(18012π)=18012π−1803⋅3!123π3+1805⋅5!125π5=0.207912 .
2.Let's find out where do x=y2 and x=2−y intercept:
y2=2−y
y2+y−2=0
y1=−2,y2=1
For every y from -2 to 1 we have y2≤2−y (we just need to check in one point, let's say y=0), so the area is bounded by the line x=2-y in the top and the line x=y2 in the bottom and y varies from -2 to 1.
∫−21dy∫y22−y(6x+2y2)dx=∫−21(3x2+2y2x)∣y22−ydy=
=∫−21(3⋅(2−y)2+2y2(2−y)−3y4−2y4)dy=
=∫−21(12−12y+3y2+4y2−2y3−5y4)dy=
=∫−21(−5y4−2y3+7y2−12y+12)dy=
=(−y5−2y4+37y3−6y2+12y)∣−21=
=−1−21+37−6+12−32+8+37⋅8+24+24=2103=51.5
Answer is 51.5
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Conductors: Sketch and label the energy band diagrams for an insulator, a semiconductor and a metal. Indicate on each diagram the energy gap, the Fermi energy and the occupied energy levels at room temperature, T=300K. Give an example of each type of material and provide an estimate of the typical energy gap in electron volts for each
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