Q. вычислить ∫L(x+y)dL, где L - правый лепесток r2=a2cos(2φ)
Convert to Polar Coordinates: Let's first express the integral in polar coordinates since the given curve is already in polar form. In polar coordinates, x=rcos(φ) and y=rsin(φ). The curve L is defined by r2=a2cos(2φ), which simplifies to r=acos(2φ) for the right petal. We need to find the bounds for φ that correspond to the right petal.
Find Bounds for φ: The right petal of the curve r2=a2cos(2φ) corresponds to the values of φ for which cos(2φ) is positive. This occurs when 2φ is between −2π and 2π, which means φ is between −4π and 4π. These are the bounds for our integral.
Compute dφdr: Now we can set up the integral in polar coordinates. The differential arc length in polar coordinates is given by dL=r2+(dφdr)2dφ. We need to compute dφdr for our curve.
Simplify Expression for dL: Differentiating r with respect to φ, we get dφdr=dφd(acos(2φ))=a(−sin(2φ))/cos(2φ). We need to square this and add it to r2 to find the expression for dL.
Write Integral in Polar Coordinates: Squaring dφdr, we get (dφdr)2=a2sin2(2φ)/cos(2φ). Adding this to r2, we get r2+(dφdr)2=a2cos(2φ)+a2sin2(2φ)/cos(2φ)=a2cos(2φ)+a2tan2(2φ).
Substitute r and Simplify: We can simplify the expression for dL using the identity 1+tan2(φ)=sec2(φ). So, r2+(dφdr)2=a2cos(2φ)+a2tan2(2φ)=a2sec2(2φ). Therefore, dL=asec2(2φ)dφ.
Integrate the Expression: Now we can write the integral of (x+y) along the curve L in polar coordinates as ∫(rcos(φ)+rsin(φ))sec2(2φ)dφ from φ=−4π to φ=4π.
Evaluate the Integral: Substituting r=acos(2φ), the integral becomes ∫φ=−4πφ=4π(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ.
Evaluate the Integral: Substituting r=acos(2φ), the integral becomes ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ from φ=−4π to φ=4π.We can simplify the integral by noting that sec2(2φ)=∣sec(2φ)∣. Since we are integrating over the range where cos(2φ) is positive, we can drop the absolute value and write sec2(2φ) as sec(2φ).
Evaluate the Integral: Substituting r=acos(2φ), the integral becomes ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ from φ=−4π to φ=4π.We can simplify the integral by noting that sec2(2φ)=∣sec(2φ)∣. Since we are integrating over the range where cos(2φ) is positive, we can drop the absolute value and write sec2(2φ) as sec(2φ).The integral simplifies to ∫acos(2φ)(cos(φ)+sin(φ))sec(2φ)dφ from φ=−4π to φ=4π. We can now integrate this expression with respect to ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ1.
Evaluate the Integral: Substituting r=acos(2φ), the integral becomes ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ from φ=−4π to φ=4π.We can simplify the integral by noting that sec2(2φ)=∣sec(2φ)∣. Since we are integrating over the range where cos(2φ) is positive, we can drop the absolute value and write sec2(2φ) as sec(2φ).The integral simplifies to ∫acos(2φ)(cos(φ)+sin(φ))sec(2φ)dφ from φ=−4π to φ=4π. We can now integrate this expression with respect to ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ1.The integral ∫acos(2φ)(cos(φ)+sin(φ))sec(2φ)dφ is not straightforward to integrate directly. We may need to use a substitution or simplify the integrand further. However, we notice that ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ3, so the integral simplifies to ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ4.
Evaluate the Integral: Substituting r=acos(2φ), the integral becomes ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ from φ=−4π to φ=4π.We can simplify the integral by noting that sec2(2φ)=∣sec(2φ)∣. Since we are integrating over the range where cos(2φ) is positive, we can drop the absolute value and write sec2(2φ) as sec(2φ).The integral simplifies to ∫acos(2φ)(cos(φ)+sin(φ))sec(2φ)dφ from φ=−4π to φ=4π. We can now integrate this expression with respect to ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ1.The integral ∫acos(2φ)(cos(φ)+sin(φ))sec(2φ)dφ is not straightforward to integrate directly. We may need to use a substitution or simplify the integrand further. However, we notice that ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ3, so the integral simplifies to ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ4.Integrating ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ4 from φ=−4π to φ=4π, we get ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ8 evaluated from φ=−4π to φ=4π.
Evaluate the Integral: Substituting r=acos(2φ), the integral becomes ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ from φ=−4π to φ=4π.We can simplify the integral by noting that sec2(2φ)=∣sec(2φ)∣. Since we are integrating over the range where cos(2φ) is positive, we can drop the absolute value and write sec2(2φ) as sec(2φ).The integral simplifies to ∫acos(2φ)(cos(φ)+sin(φ))sec(2φ)dφ from φ=−4π to φ=4π. We can now integrate this expression with respect to ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ1.The integral ∫acos(2φ)(cos(φ)+sin(φ))sec(2φ)dφ is not straightforward to integrate directly. We may need to use a substitution or simplify the integrand further. However, we notice that ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ3, so the integral simplifies to ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ4.Integrating ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ4 from φ=−4π to φ=4π, we get ∫(acos(2φ)cos(φ)+acos(2φ)sin(φ))sec2(2φ)dφ8 evaluated from φ=−4π to φ=4π.Evaluating the antiderivative at the bounds, we get φ=−4π1.
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