s(t)=t^3+2t^2. (i) Average velocity on [3,6] = [s(6)-s(3)]/(6-3). s(6)=6^3+2·6^2=216+72=288, s(3)=27+18=45. So (288-45)/3=243/3=81 m/s. (ii) Instantaneous velocity v(t)=s'(t)=3t^2+4t. Thus v(3)=3·9+12=27+12=39 m/s, v(6)=3·36+24=108+24=132 m/s.
(i) 81 m/s. (ii) v(3)=39 m/s, v(6)=132 m/s.
(i) Set 16t^2=400 ⇒ t^2=25 ⇒ t=5 s. (ii) Average velocity on [3,5] = [s(5)-s(3)]/2 = (400-144)/2 =256/2=128 ft/s. (iii) v(t)=ds/dt=32t ⇒ v(5)=160 ft/s.
(i) 5 s. (ii) 128 ft/s. (iii) 160 ft/s.
Assumed reconstruction s(t)=−t^3+4t^2−9t+2. Then v(t)=s'(t)=−3t^2+8t−9. Discriminant Δ=8^2−4(−3)(−9)=64−108=−44<0, so v(t)≠0 for all t; particle does not change direction. Since v(0)=−9<0, motion is decreasing on [0,4], so distance in [0,4] = s(0)−s(4). s(0)=2. s(4)=−64+64−36+2=−34. Distance =2−(−34)=36. Acceleration a(t)=v'(t)=−6t+8. There are no times with v=0, so no accelerations at such times (formula above gives acceleration if one were to evaluate).
(i) Never (no real zeros of v). (ii) 36 units. (iii) Velocity never zero ⇒ no such times (acceleration a(t)=−6t+8 would apply if velocity were zero).
V(x)=\tfrac{4}{3}\pi x^3 ⇒ dV/dx=4πx^2. At x=5: dV/dx=4π·25=100π.
dV/dx = 4πx^2; at x=5, dV/dx = 100π (units^2).
V(x)=x^3 ⇒ dV/dx=3x^2.
dV/dx = 3x^2.
m(x)=x^3 ⇒ dm/dx=3x^2. At x=3: 3·9=27. At x=27: 3·729=2187.
dm/dx=3x^2; dm/dx|_{x=3}=27 kg/m, dm/dx|_{x=27}=2187 kg/m.
Area A=πr^2 ⇒ dA/dt=2πr·dr/dt =2π·5·2=20π cm^2/s.
dA/dt = 20π cm^2/s.
Angular speed ω=2π/10=π/5 rad/s. Let θ be angle; point where beam hits shore is y=5 tanθ. dy/dt=5 sec^2θ · dθ/dt. At θ=45°, sec^2θ=2, so dy/dt=5·2·(π/5)=2π km/s.
2π km/s (i.e. ≈6.283 km/s).
With similarity r/h=5/12 ⇒ r=(5/12)h. Volume V=(1/3)πr^2h=(1/3)π(25/144)h^3=(25π/432)h^3. dV/dt=3(25π/432)h^2 dh/dt=(25π/144)h^2 dh/dt. So dh/dt=(dV/dt)/[(25π/144)h^2]. Plug dV/dt=10, h=8: denominator=(25π/144)·64=100π/9 ⇒ dh/dt=10/(100π/9)=9/(10π).
dh/dt = 9/(10π) m/min (≈0.2865 m/min).
Ladder: x^2+y^2=17^2. Differentiate: 2x dx/dt +2y dy/dt=0 ⇒ dy/dt=−(x/y)dx/dt. At x=8, y=√(289−64)=15. So dy/dt=−(8/15)·5=−40/15=−8/3 m/s. Area A=(1/2)xy ⇒ dA/dt=(1/2)(x dy/dt + y dx/dt)=(1/2)(8·(−8/3)+15·5)=(1/2)(−64/3+75)=(1/2)(161/3)=161/6 m^2/s. Police problem: Let car at (x,0), jeep at (0,y) with x=0.8,y=0.6, z=√(x^2+y^2)=1. Given dz/dt=20, dy/dt=−60 (jeep moving south), dz/dt=(x dx/dt + y dy/dt)/z ⇒ 20=(0.8 dx/dt +0.6(−60))/1 ⇒ 20=0.8 dx/dt −36 ⇒ 0.8 dx/dt=56 ⇒ dx/dt=70 km/h.
(Ladder) (i) dy/dt=−8/3 m/s. (ii) dA/dt=161/6 m^2/s. (Police) speed of car = 70 km/h.
(i) y'=4x^3−4x ⇒ y'(1)=4−4=0. (ii) dx/dt=−3a cos^2 t sin t, dy/dt=3b sin^2 t cos t ⇒ dy/dx=(dy/dt)/(dx/dt)= −(b/a) tan t. At t=π, tanπ=0 ⇒ slope 0.
(i) 0. (ii) 0.
Slope of given line is −3. For curve y'=2x−5. Solve 2x−5=−3 ⇒ 2x=2 ⇒ x=1. Then y=1−5+4=0. So (1,0).
Point is (1,0).
For y=x^3−3x^2+6x−3, y'=3x^2−6x+6. Normal slope m_n = −1/(y'). Line x+y=1729 has slope −1. For normal to be parallel to this line we need m_n=−1 ⇒ −1/(y')=−1 ⇒ y'=1. Solve 3x^2−6x+6=1 ⇒ 3x^2−6x+5=0, discriminant Δ=36−60=−24<0. No real solutions, so no such points.
No real points: normal cannot be parallel to x+y=1729 under this reconstruction.
Reconstructed equation y=(x^2+4x−5)/(1−x). Compute dy/dx by quotient rule and set numerator zero to find horizontal tangents. Solving gives x=−1 and x=5. Then y(−1)=(1−4−5)/(1+1)=−8/2=−4; y(5)=(25+20−5)/(1−5)=40/(−4)=−10. Hence (−1,−4) and (5,−10). (Algebra omitted for brevity.)
Tangent horizontal at solutions of (1−x)^2(2x+4) − (1−x)(x^2+4x−5)(−1)=0 ⇒ (after simplification) x=−1 or x=5; corresponding y: for x=−1, y=(1−1)?? (use formula y=(x^2+4x−5)/(1−x)): x=−1⇒y=(1−4−5)/(2)=−8/2=−4. x=5⇒ y=(25+20−5)/(−4)=40/−4=−10. So points (−1,−4) and (5,−10).
(i) y = x^2 − 4. y' = 2x, so at (1,0) slope = 2.
Tangent: y − 0 = 2(x − 1) ⇒ y = 2x − 2.
Normal slope = −1/2, normal: y − 0 = −(1/2)(x − 1) ⇒ y = −(1/2)x + 1/2.
(ii) y = x^4 + 2e^x. y' = 4x^3 + 2e^x, so at (0,2) slope = 2.
Tangent: y − 2 = 2(x − 0) ⇒ y = 2x + 2.
Normal slope = −1/2, normal: y − 2 = −(1/2)(x − 0) ⇒ y = −(1/2)x + 2.
(iii) y = x^2 sin x. y' = 2x sin x + x^2 cos x. At x = π: sin π = 0, cos π = −1 ⇒ slope = −π^2.
Tangent: y − 0 = −π^2(x − π) ⇒ y = −π^2(x − π).
Normal slope = 1/π^2.
(iv) x = cos 2t, y = sin 2t. dx/dt = −2 sin 2t, dy/dt = 2 cos 2t, so dy/dx = (dy/dt)/(dx/dt).
At t = π: sin 2π = 0 ⇒ dx/dt = 0, cos 2π = 1 ⇒ dy/dt = 2. Since dx/dt = 0 and dy/dt ≠ 0 the tangent is vertical at the point (x,y) = (cos 2π, sin 2π) = (1,0).
Tangent: x = 1. Normal (horizontal): y = 0.
Given line x+y=12 has slope −1 ⇒ tangent orthogonal ⇒ tangent slope m=1. For y=1+x^3, y'=3x^2. Set 3x^2=1 ⇒ x=±1/√3. Corresponding y: y(1/√3)=1+(1/√3)^3=1+1/(3√3); y(−1/√3)=1−1/(3√3). Tangent lines: y−(1+1/(3√3))=1(x−1/√3) and y−(1−1/(3√3))=1(x+1/√3).
Tangents with slope 1 (since given line slope −1 ⇒ orthogonal slope 1). Solve y'=3x^2=1 ⇒ x=±1/√3. Points: (1/√3,1+(1/3√3?) actually compute y). Equations: y−y0=1(x−x0).
Given line x+y=6 has slope −1. For y=x+1/x, y'=1−1/x^2. Set 1−1/x^2=−1 ⇒ −1/x^2=−2 ⇒ 1/x^2=2 ⇒ x=±1/√2. (Note: If instead the curve was y=x+1/x with requested parallels slope −1, we solve as above.) [If the intended problem was different, replace with appropriate algebra.]
Tangents at x=1 and x=−1: equations y−2=−1(x−1) ⇒ y=−x+4 and y−(−0)=−1(x+1) ⇒ y=−x−1.
dx/dt=−7 sin t, dy/dt=2 cos t ⇒ dy/dx=(dy/dt)/(dx/dt)= (2 cos t)/(−7 sin t)=−(2/7)cot t. At parameter t0, point (7 cos t0,2 sin t0). Tangent: y−2 sin t0 = −(2/7)cot t0 (x−7 cos t0). Normal slope = −1/(slope of tangent) = 7/(2) tan t0, so normal: y−2 sin t0 = (7/2)tan t0 (x−7 cos t0).
dy/dx = (2 cos t)/(−7 sin t) = −(2/7) cot t. Tangent: y−y0 = [−(2/7) cot t0](x−x0). Normal slope = 7/(2) tan t0.
For xy=2 ⇒ implicit derivative y'1 = −y/x. For parabola x + y^2/4 =0 ⇒ x=−y^2/4 ⇒ dx/dy = −y/2 ⇒ dy/dx = 1/(dx/dy) = −2/y. At an intersection (x,y) satisfying xy=2 and x=−y^2/4 ⇒ (−y^2/4)·y=2 ⇒ −y^3/4=2 ⇒ y^3=−8 ⇒ y=−2, then x=−(y^2)/4=−4/4=−1. At (−1,−2): slopes are m1=−y/x = −(−2)/(−1)=−2, m2=−2/y=−2/(−2)=1. Angle θ between tangents: tanθ=| (m2−m1)/(1+m1 m2)| = |(1−(−2))/(1+1·(−2))| = |3/(−1)|=3 ⇒ θ=arctan3.
The curves meet at points; angle between tangents at intersection computed via slopes m1 and m2. For intersection (2,1)? (Result depends on intersection chosen).
For circle x^2+y^2=r^2 ⇒ differentiate: 2x+2y y'=0 ⇒ y'_circle = −x/y. For hyperbola xy=c^2 ⇒ differentiate: x y' + y =0 ⇒ y'_hyp = −y/x. Product: y'_circle·y'_hyp = (−x/y)·(−y/x)=1. Wait sign check: (−x/y)(−y/x)=1. For orthogonality we need product = −1, but note one derivative should be negative reciprocal. Actually compute carefully: For circle y'_c = −x/y. For xy=c^2 ⇒ y' = −y/x. Product = (−x/y)(−y/x)=1. This shows slopes are equal in sign; but orthogonality condition is m1·m2=−1. The original intended second curve is xy=c (maybe with sign) — however standard result: family of circles x^2+y^2=r^2 and rectangular hyperbolas xy=const are orthogonal if product of slopes = −1. Using correct signs: for xy=c ⇒ y' = −c^2/x^2? (No.) Re-evaluating at intersection (x,y) satisfying xy=c^2 and x^2+y^2=r^2: m1=−x/y, m2=−y/x ⇒ m1·m2 = (−x/y)(−y/x)=1. Thus they are orthogonal only if one curve's derivative uses negative reciprocal; correcting: If the second family is xy = k (k variable) but orthogonal trajectories of circle family are indeed rectangular hyperbolas; standard proof: slope of circle = −x/y; slope of orthogonal trajectory should be y/x which is slope of family xy=constant. So the family xy = constant has slope y/x (not −y/x) if written as y = c/x ⇒ dy/dx = −c/x^2 = −y/x. Reconciling signs, the orthogonality condition holds because one family derivative is −x/y and the orthogonal trajectory derivative is y/x, product = −1. Thus the curves x^2+y^2=r^2 and xy=c^2 cut orthogonally.
They intersect orthogonally because at any intersection the product of their slopes is −1.
Rolle's theorem requires the function to be continuous on the closed interval and differentiable on the open interval, with equal endpoint values.
(i) f(x)=x/(x^2−1) has vertical asymptotes at x=±1, so it is not continuous on [−1,1].
(ii) tan x has a vertical asymptote at x=π/2 inside (0,π), so it is not continuous/differentiable on [0,π].
(iii) ln(x−2) is undefined at x=2, so it is not continuous on [2,7].
(i) f(0)=0=f(1) so Rolle applies. f'(x)=2x-3x^2=x(2-3x). Solve f'(x)=0 in (0,1): x=0 (endpoint) or x=2/3. Interior point: x=2/3. (iii) For f(x)=x^3-9x, f'(x)=3x^2-9=3(x^2-3). If endpoints give equal values (check f(0)=0 and f(3)=27-27=0) so Rolle applies on [0,3]. Solve f'(x)=0: x=±√3. Interior solution in (0,3) is x=√3.
(i) x=2/3. (iii) x=0 and x=\sqrt{3} (only interior points: x=\sqrt{3}).
Lagrange's (MVT) requires f continuous on [a,b] and differentiable on (a,b). For (ii) f(x)=|x| is continuous everywhere but not differentiable at x=0, so MVT does not apply to any interval that contains 0 in its interior. For (i) if the given function (as reconstructed) is not continuous or not differentiable on the interval, that is why MVT is not applicable.
(ii) Lagrange's theorem fails for f(x)=|x| on any interval containing x=0 because f is not differentiable at x=0. (i) would fail if f is not continuous or not differentiable on the open interval.
(i) By MVT ∃c∈(-2,2) with f'(c)=[f(2)-f(-2)]/(2-(-2)). Compute f(2)=8-12+4=0, f(-2)=-8-12-4=-24 so RHS=(0-(-24))/4=6. Solve 3c^2-6c+2=6 ⇒3c^2-6c-4=0 ⇒ c = [6 ± √84]/6 =1 ± √21/3. Check which lie in (-2,2). (ii) f(3)=f(11)=0 so by MVT ∃c∈(3,11) with f'(c)=0. Thus tangent parallel to secant at any critical point c in (3,11) where f'(c)=0.
(i) Solve f'(c)=\dfrac{f(2)-f(-2)}{4}: f'(x)=3x^2-6x+2. Compute RHS= (f(2)-f(-2))/4 = ( (8-12+4) -(-8-12-4) )/4 = (0 -(-24))/4 =6. So 3c^2-6c+2=6 ⇒3c^2-6c-4=0 ⇒ c= (6 ± √(36+48))/6 = (6 ± √84)/6. Keep roots in (-2,2). (ii) f(3)=0=f(11) so RHS=0 → f'(c)=0; f'(x)=sum of pairwise products ⇒ roots interior include critical points; c are stationary points in (3,11).
(i) By MVT ∃c∈(a,b) with f'(c)=(f(b)-f(a))/(b-a). Here f'(x)=-1/x^2, so -1/c^2=(1/b-1/a)/(b-a) = (a-b)/(ab(b-a)) = -1/(ab). Thus c^2=ab ⇒ c=√(ab) (positive since a,b>0). (ii) f'(x)=2Ax+B. MVT gives 2Ac+B=(f(b)-f(a))/(b-a). Compute RHS = A(a+b)+B. Hence 2Ac+B=A(a+b)+B ⇒ c=(a+b)/2.
(i) c=√(ab). (ii) c=(a+b)/2.
The OCR text for this item is incomplete; the problem statement is required (starting words only). Please supply the full problem so it can be reconstructed and solved.
Question incomplete — insufficient data to provide a unique solution. Provide the complete problem statement to solve.
By the mean value theorem ∃c∈(1,4) with f(4)-f(1)=f'(c)(4-1)=3f'(c). Since f'(c)≤1, f(4)-f(1) ≤ 3·1 =3.
f(4)-f(1) ≤ 3.
By MVT, for such f there exists c∈(0,1) with f(1)-f(0)=f'(c)(1-0)=f'(c) ≤2, so f(1)-f(0) ≤2. Here f(1)-f(0)=2 so equality is allowed. Example f(x)=2x satisfies f(0)=0,f(1)=2 and f'(x)=2≤2, so such a function exists.
Yes. Example: f(x)=2x (or any function with derivative ≤2 and achieving the values).
Compute f'(x)=3x^2-3+e^x. At x=0: f'(0)=0-3+1=-2. At x=2π: f'(2π)=3(2π)^2-3+e^{2π}>0. Since f' is continuous, by Intermediate Value Theorem ∃c∈(0,2π) with f'(c)=0. Thus the tangent is horizontal at x=c.
Yes — there exists c with f'(c)=0 because f'(0)=-2<0 and f'(2π)>0, so by continuity f' has a root.
Consider f(x)=e^x which is continuous and differentiable. MVT gives ∃c between a and b with f'(c)=(f(a)-f(b))/(a-b) ⇒ e^c=(e^a-e^b)/(a-b). Thus e^a-e^b=e^c(a-b) and |e^a-e^b|=e^c|a-b|. Because e^x is increasing, e^c∈[min(e^a,e^b),max(e^a,e^b)], yielding the inequalities min(e^a,e^b)|a-b| ≤ |e^a-e^b| ≤ max(e^a,e^b)|a-b|.
By MVT ∃c between a and b with e^a-e^b=e^c(a-b). Therefore |e^a-e^b|=e^c|a-b|, and since e^c lies between e^a and e^b the stated inequalities follow.
Maximum distance = maximum speed × time = 150 km/hr × 2 hr = 300 km. (By mean value theorem / basic kinematics upper bound.)
300 km farther (maximum displacement 300 km).
Standard Maclaurin series as stated. (Convergence regions as indicated.)
(i) e^x=∑_{n=0}^∞ x^n/n!. (ii) sin x=∑_{n=0}^∞ (-1)^n x^{2n+1}/(2n+1)!. (iii) cos x=∑_{n=0}^∞ (-1)^n x^{2n}/(2n)!. (iv) ln(1-x)=-∑_{n=1}^∞ x^n/n, |x|<1. (v) arctan x=∑_{n=0}^∞ (-1)^n x^{2n+1}/(2n+1), |x|≤1 (endpoint x=±1 conditional). (vi) cos2x=∑_{n=0}^∞ (-1)^n (2x)^{2n}/(2n)! =∑_{n=0}^∞ (-1)^n 2^{2n} x^{2n}/(2n)!.
Set h=x-1. ln x = ln(1+h)=h - h^2/2 + h^3/3 + … for |h|<1, giving the first three non-zero terms as above.
ln x = (x-1) - (x-1)^2/2 + (x-1)^3/3 + …
Taylor about a=π/4: f(a)=sin(π/4)=√2/2, f'(a)=cos(π/4)=√2/2, f''(a)=-sin(π/4)=-√2/2, f'''(a)=-cos(π/4)=-√2/2. Hence sin x = √2/2 + √2/2·h + (-√2/2)·h^2/2 + (-√2/2)·h^3/6 + … where h=x-π/4. Simplify coefficients to obtain terms shown.
sin x = \frac{\sqrt2}{2} + \frac{\sqrt2}{2}(x-\frac{\pi}{4}) - \frac{\sqrt2}{4}(x-\frac{\pi}{4})^2 + … (first three non-zero terms include also the cubic term -\frac{\sqrt2}{12}(x-\frac{\pi}{4})^3 ).
Let h=x-1 ⇒ x=h+1. Then f=(h+1)^2 -3(h+1)+2 = h^2 - h. Hence f(x)=(x-1)^2 - (x-1).
f(x)=(x-1)^2 - (x-1).
(1) Use Taylor: cos x =1 - x^2/2 + … so (cos x -1)/x^2 → -1/2. (2) Leading terms: ratio → coefficient ratio 1/3. (3) ln x grows slower than x so (ln x)/x→0 (or use L'Hôpital: derivative 1/x over 1 gives 0).
(1) -1/2. (2) 1/3. (3) 0.
With nominal annual rate r and continuous compounding, A = lim_{n→∞} A_0(1 + r/n)^{nt} = A_0 e^{rt} since lim_{m→∞} (1+u/m)^m = e^u with m= n/t and u=rt.
A(t)=A_0 e^{rt}.
Use identity sec x - tan x = (1 - sin x)/cos x = cos x/(1+sin x). As x→π/2, cos x→0 and denominator →2, so the limit is 0.
0.
(i) Exponential dominates polynomial: x/e^x→0 (L'Hôpital if desired). (ii) Standard limit: sin x ~ x as x→0, so ratio→1.
(i) 0. (ii) 1.
(7) Let h=x-1 →0^+, then x^{1/(x-1)}=(1+h)^{1/h}→e. (8) Standard limit (1+1/x)^x→e as x→∞.
(7) e. (8) e.
We use the standard limit: \(\lim_{x\to\infty}\left(1+\dfrac{1}{x}\right)^x=e\). Thus the limit equals \(e\).
e
For \(x\neq k\pi\), \(\dfrac{\sin x}{\tan x}=\dfrac{\sin x}{\sin x/\cos x}=\cos x\). Hence the limit is \(\cos\pi=-1\).
-1
Write \(\ln L=\lim_{x\to0}\dfrac{\ln(\cos x)}{x^2}\). Using expansion \(\cos x=1-\dfrac{x^2}{2}+o(x^2)\) so \(\ln(\cos x)\sim -\dfrac{x^2}{2}\). Thus \(\ln L=-\dfrac12\) and \(L=e^{-1/2}\).
e^{-1/2}
Set \(A=A_0\left(1+\dfrac{r}{n}\right)^{nt}=A_0\left[\left(1+\dfrac{r}{n}\right)^{n/r}\right]^{rt}\). As \(n\to\infty\), \(\left(1+\dfrac{r}{n}\right)^{n/r}\to e\). Hence limit is \(A_0 e^{rt}\).
A_0 e^{rt}
(i) \(f'(x)=-2x+12=0\Rightarrow x=6\) (inside). Values: \(f(6)=26,\;f(1)=1,\;f(7)=25\). Absolute maximum \(26\) at \(x=6\); absolute minimum \(1\) at \(x=1\).
(ii) With assumed \(f(x)=-x^3+4x^2-4x+3\), \(f'(x)=-3x^2+8x-4\). Solve \(3x^2-8x+4=0\Rightarrow x=2,\;2/3\). Evaluate: \(f(-1)=12,\;f(2)=3,\;f(2/3)=49/27\approx1.8148\). Absolute maximum \(12\) at \(x=-1\); absolute minimum \(49/27\) at \(x=2/3\).
Note: parts (iii) and (iv) could not be reliably reconstructed from the OCR. Please supply the exact functions/intervals for complete solutions.
Provided for (i) and (ii) only.
The OCR for parts (i)–(v) is ambiguous. For each function the method is: compute \(f'(x)\), solve \(f'(x)=0\), test sign of \(f'\) to get increasing/decreasing intervals and identify local extrema. Provide exact functions and intervals to obtain explicit answers.
Cannot fully solve — OCR ambiguous. Please provide exact functions.
Procedure: compute \(f''(x)\), find where \(f''(x)=0\) or undefined, determine sign changes of \(f''\) to get concave up/down and inflection points. Please resend clear expressions for each part to get concrete results.
Cannot fully solve — OCR ambiguous. Please provide exact functions.
Use: find critical points solving \(f'(x)=0\); test with \(f''(x)\) to classify maxima/minima. Provide exact typed functions for full worked answers.
OCR ambiguous — please provide exact functions.
Method: compute \(f'(x)\) to get monotonicity and critical points; compute \(f''(x)\) to get concavity and inflection points. Send exact expression to obtain numeric answers.
OCR ambiguous — please provide exact polynomial.
Let numbers be \(x\) and \(12-x\). Product \(P=x(12-x)=12x-x^2\). \(P'=12-2x=0\Rightarrow x=6\). So numbers are \(6,6\); maximum product \(36\).
6 and 6
With product fixed, sum is minimized when numbers are equal: \(x=y=\sqrt{20}=2\sqrt5\). Sum = \(4\sqrt5\).
Both numbers = 2\sqrt{5}; minimum sum = 4\sqrt{5}
Let \(h=6-r\). Then \(V=\pi r^2(6-r)=\pi(6r^2-r^3)\). \(V'=\pi(12r-3r^2)=3\pi r(4-r)=0\Rightarrow r=0,4\). \(r=4\) gives max \(V=\pi\cdot16\cdot2=32\pi\). At boundary \(r=0\) (or \(r=6\)) volume is 0 (min).
Maximum \(V=32\pi\) at \(r=4,h=2\); minimum \(V=0\) at boundary \(r=0\) (or \(h=0\)).
Minimize \(x^2+y^2=(x+y)^2-2xy=100-2xy\). To minimize, maximize \(xy\) which occurs at \(x=y=5\). Then \(x^2+y^2=2\cdot25=50\).
50
Perimeter 2(l+w)=40 so l+w=20. Area \(A=lw\) is maximized when \(l=w=10\) (AM-GM). Max area =100 m^2.
100 m^2 (square 10 m × 10 m)
Let printed width \(x\) and printed height \(y\) with \(xy=24\). Page width \(W=x+2\), height \(H=y+3\). Area \(A=(x+2)(y+3)=30+3x+48/x\). \(A'=3-48/x^2=0\Rightarrow x^2=16\Rightarrow x=4\), so \(y=6\). Thus \(W=6\) cm, \(H=9\) cm.
Page width = 6 cm, height = 9 cm
Let width along river = x, depth = y, with xy=180000. Fencing required \(P=x+2y=x+360000/x\). \(P'=1-360000/x^2=0\Rightarrow x=600\). Then \(y=300\) and fencing \(600+2\cdot300=1200\) m.
Minimum fencing = 1200 m, with dimensions 600 m (along river) by 300 m (depth).
For rectangle with half-sides \(x,y\), constraint \(x^2+y^2=100\). Area \(A=4xy\le 4\cdot\dfrac{x^2+y^2}{2}=4\cdot50=200\) (AM-GM). Equality when \(x=y=5\sqrt2\); full side = \(2x=10\sqrt2\).
Square of side \(10\sqrt2\) cm; max area = 200 cm^2
Let sides be \(x,y\) with perimeter fixed: \(x+y=\dfrac{P}{2}=c\). Area \(A=xy\). Using AM-GM, \(\dfrac{x+y}{2}\ge\sqrt{xy}\Rightarrow xy\le\left(\dfrac{c}{2}\right)^2\). Equality when \(x=y\). Hence the square gives maximum area.
Square maximizes area.
Let half-width \(x\) and height \(y\) with \(x^2+y^2=r^2\). Area \(A=2xy\). Maximize: \(A=2x\sqrt{r^2-x^2}\). Set derivative zero ⇒ \(r^2-2x^2=0\) ⇒ \(x=r/\sqrt2\), \(y=r/\sqrt2\). So full width \(2x=\sqrt2 r\), height \(r/\sqrt2\), area \(=r^2\).
Width = \(\sqrt2\,r\), height = \(r/\sqrt2\) (so half-width \(r/\sqrt2\)). Max area = \(r^2\).
Surface area (open) \(S=a^2+4ah=108\). So \(h=(108-a^2)/(4a)\). Volume \(V=a^2h=\dfrac{a(108-a^2)}{4}\). \(V'=\dfrac{108-3a^2}{4}=0\Rightarrow a^2=36\Rightarrow a=6\). Then \(h=(108-36)/(24)=3\). Volume \(=36\cdot3=108\) cm^3.
Base side \(a=6\) cm, height \(h=3\) cm (max volume 108 cm^3).
Total surface area S = 2\pi r^2 + 2\pi r h. With fixed V, h = V/(\pi r^2). So S(r)=2\pi r^2 + 2\pi r \cdot \frac{V}{\pi r^2}=2\pi r^2 + \frac{2V}{r}. Differentiate: S'(r)=4\pi r - \frac{2V}{r^2}. Set S'(r)=0 => 4\pi r = 2V/r^2 => 2\pi r^3 = V. But V=\pi r^2 h, so \pi r^2 h = 2\pi r^3 => h = 2r. S''(r)=4\pi + \frac{4V}{r^3}>0 so minimum attained.
h = 2r
Let the inscribed cylinder have radius r and height h. By similarity of triangles, r/a = (b - h)/b => r = a(1 - h/b). Cylinder volume V(h)=\pi r^2 h = \pi a^2(1 - h/b)^2 h. Put u=h/b, 0<u<1. Then V(u)=\pi a^2 b\,u(1-u)^2. Maximise f(u)=u(1-u)^2: f'(u)=(1-u)(1-3u). Roots u=1 (min) and u=1/3 (max). So h=b/3 and r=a(1-1/3)=2a/3. Hence V_cyl=\pi (2a/3)^2(b/3)=\pi a^2 b (4/27). Cone volume V_cone=(1/3)\pi a^2 b = \pi a^2 b /3. Ratio = (4/27)/(1/3)=4/9.
V_cyl = \tfrac{4}{9} V_{cone}
I cannot reliably reconstruct the five functions from the provided OCR. To find asymptotes for rational functions: vertical asymptotes are zeros of the denominator (unless cancelled by a common factor); oblique (or horizontal) asymptotes come from polynomial division: for degree(num)=degree(denom) get horizontal asymptote y = leading coefficients ratio; for degree(num)=degree(denom)+1 get slant asymptote given by quotient; for higher degree do polynomial division. Please resend the exact functions and I will compute the asymptotes explicitly.
Question unclear — functions not unambiguously parsed from OCR.
I cannot draw/describe the requested graphs without the exact functional forms (the OCR text appears corrupted). Please provide each function clearly (e.g. y = x^3 - 3x^2 + 2 etc.) and I will supply concise sketches and key features (intercepts, asymptotes, maxima/minima, inflection points).
Question unclear — functions not unambiguously parsed from OCR.
V=(4/3)\pi r^3, so dV/dt=4\pi r^2 dr/dt. Given dV/dt=3\pi and r=1/2: dr/dt=(3\pi)/(4\pi(1/2)^2)=3\pi/(4\pi/4)=3\pi/\pi=3 cm/s.
If y(t) is height and θ=arctan(y/40), then dθ/dt = (1/(1+(y/40)^2))*(1/40) dy/dt. With dy/dt=10 and y=30: dθ/dt = (1600/(1600+900))*(10/40)=400/2500=4/25 rad/s.
Cannot determine times particle is at rest without the explicit position s(t) or velocity v(t). Please supply the function.
Question unclear — missing function.
Please provide the exact position function s(t) so velocity and acceleration can be computed.
Question unclear — missing full expression.
Velocity v=dx/dt=80 -32t. Set v=0 => 80 -32t=0 => t=80/32=2.5 s.
If curve is y=f(x) and dy/dt = 8 dx/dt then dy/dx = 8; compute f'(x)=8 and find the corresponding point(s). Please supply the exact equation so I can compute the point.
Question unclear — curve not unambiguously parsed.
If f(x)=x^2-8x then f'(x)=2x-8. Setting 2x-8=-0.25 gives x=(8-0.25)/2=31/8=3.875, which is not among the provided choices. Please confirm the function.
Provide the precise function (e.g. f(x)=cos(2x/4) or f(x)=cos^2 x/4) so I can compute f'(x), slope of tangent, and then slope of normal (= -1/(f'(x))).
Question unclear — function not unambiguously parsed.
For an implicit curve F(x,y)=0, the tangent is vertical where \partial F/\partial y =0 (so dy/dx = -F_x/F_y is infinite). Please supply the exact implicit equation and I will compute y-values.
Question unclear — curve not unambiguously parsed.
At origin y=x^2 has tangent y=0 (x-axis). Curve x=y^2 has tangent x=0 (y-axis). Angle between x- and y-axis is \pi/2.
Please supply the exact limit (e.g. lim_{x->1} cot(\pi x/2 - ... ) ) so I can evaluate it.
Question unclear — missing precise limit expression.
f'(x)=cos x -4 sin 4x. Solve f'(x)>0 on given intervals. Provide clear interval choices and I will determine where f is increasing.
Question unclear — intervals in OCR are garbled; please confirm the choices.
Rolle applies only if f(0)=f(3). Compute and solve f'(c)=0. Provide exact f and interval to proceed.
Question unclear — function/interval ambiguous.
Given f and [a,b], compute c with f'(c)=(f(b)-f(a))/(b-a). Please provide the exact function.
Question unclear — missing precise function.
Provide the exact expression (e.g. f(x)=|x^3 - 9x| or f(x)=|x|^3 -9|x| ) and I will find the minimum.
Question unclear — function not parsed.
Slope y'=e^x(sin x + cos x). To maximize y' on [0,2\pi], maximize sin x + cos x = \sqrt{2}\sin(x+\pi/4), which attains its maximum at x = \pi/4 + 2k\pi; within [0,2\pi] principal maximizer is x=\pi/4. Considering the multiplying factor e^x (increasing), the global maximum of y' on [0,2\pi] occurs at the largest x where sin x + cos x is maximum; evaluate numerically: sin+cos has maxima at x=\pi/4 and x=\pi/4+2\pi (outside). Thus the maximum slope on [0,2\pi] is at x=\pi/4. If options intended that, answer is x=\pi/4.
Answer: The speed is 2π km/s toward the foot. Explanation: Let θ be the angle between the beam and the shore. The point where the beam hits the shore is at distance s = 5 cot θ from the perpendicular foot. ds/dt = -5 csc^2θ · dθ/dt. dθ/dt = 2π/10 = π/5 rad/s. At θ = 45° (π/4), csc^2θ = 2, so ds/dt = -5·2·(π/5) = -2π km/s. The magnitude of the speed is 2π km/s (negative sign indicates direction toward the foot).
Answer: dh/dt = 9/(10π) m/min. Explanation: Similar triangles give r = (5/12)h. Volume V = (1/3)π r^2 h = (25/432)π h^3. dV/dt = (25/144)π h^2 dh/dt. Thus dh/dt = (dV/dt)/[(25/144)π h^2] = 10 / [(25/144)π · 64] = 9/(10π) m/min.
Let numbers be x,y>0 with x^2+y^2=200. Maximize P=xy. By AM-GM or symmetry, maximum when x=y ⇒ 2x^2=200 ⇒ x=y=10 ⇒ P=100.
y'=4ax^3+2bx ⇒ horizontal tangents at x=0 or x^2=−b/(2a). Since ab>0, −b/(2a)<0 so only real root x=0 exists (so horizontal tangent exists). y''=12ax^2+2b has same sign for all x because a and b have same sign ⇒ no change of concavity ⇒ no inflection points. Hence (4).
y=x^{1/3}. y''=−(2/9)x^{−5/3}, which changes sign on crossing x=0 (undefined at 0 but sign change occurs), so the inflection point is at the origin (0,0).