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Here are the solutions to the calculus questions:

1. Evaluate the following limits:

b) lim⁡x→0sin⁡3xtan⁡5x\lim_{x \to 0} \frac{\sin 3x}{\tan 5x}

Step 1: Direct substitution yields sin⁡(0)tan⁡(0)=00\frac{\sin(0)}{\tan(0)} = \frac{0}{0}, an indeterminate form.

Step 2: Apply L'Hôpital's Rule by differentiating the numerator and denominator.
The derivative of sin⁡3x\sin 3x is 3cos⁡3x3 \cos 3x.
The derivative of tan⁡5x\tan 5x is 5sec⁡25x5 \sec^2 5x.

lim⁡x→03cos⁡3x5sec⁡25x\lim_{x \to 0} \frac{3 \cos 3x}{5 \sec^2 5x}

Step 3: Substitute x=0x=0 into the new expression.

3cos⁡(0)5sec⁡2(0)=3⋅15⋅12=35\frac{3 \cos(0)}{5 \sec^2(0)} = \frac{3 \cdot 1}{5 \cdot 1^2} = \frac{3}{5}

The limit is 35\boxed{\frac{3}{5}}.

c) lim⁡r→∞3r3−2rr3+5r2+1\lim_{r \to \infty} \frac{3r^3 - 2r}{r^3 + 5r^2 + 1}

Step 1: Divide every term in the numerator and denominator by the highest power of rr in the denominator, which is r3r^3.

lim⁡r→∞3r3r3−2rr3r3r3+5r2r3+1r3\lim_{r \to \infty} \frac{\frac{3r^3}{r^3} - \frac{2r}{r^3}}{\frac{r^3}{r^3} + \frac{5r^2}{r^3} + \frac{1}{r^3}}

Step 2: Simplify the expression.

lim⁡r→∞3−2r21+5r+1r3\lim_{r \to \infty} \frac{3 - \frac{2}{r^2}}{1 + \frac{5}{r} + \frac{1}{r^3}}

Step 3: Apply the limit. As r→∞r \to \infty, terms of the form crn\frac{c}{r^n} approach 0.

3−01+0+0=31=3\frac{3 - 0}{1 + 0 + 0} = \frac{3}{1} = 3

The limit is 3\boxed{3}.

2. Differentiate from first principles:

a) y=x2+3xy = x^2 + 3x

Step 1: Write the definition of the derivative from first principles.

dydx=lim⁡h→0f(x+h)−f(x)h\frac{dy}{dx} = \lim_{h \to 0} \frac{f(x+h) - f(x)}{h}

Step 2: Substitute f(x)=x2+3xf(x) = x^2 + 3x and f(x+h)=(x+h)2+3(x+h)f(x+h) = (x+h)^2 + 3(x+h).

f(x+h)−f(x)=[(x+h)2+3(x+h)]−[x2+3x]f(x+h) - f(x) = [(x+h)^2 + 3(x+h)] - [x^2 + 3x] =[x2+2xh+h2+3x+3h]−[x2+3x]= [x^2 + 2xh + h^2 + 3x + 3h] - [x^2 + 3x] =2xh+h2+3h= 2xh + h^2 + 3h

Step 3: Substitute this into the limit and simplify.

dydx=lim⁡h→02xh+h2+3hh=lim⁡h→0h(2x+h+3)h=lim⁡h→0(2x+h+3)\frac{dy}{dx} = \lim_{h \to 0} \frac{2xh + h^2 + 3h}{h} = \lim_{h \to 0} \frac{h(2x + h + 3)}{h} = \lim_{h \to 0} (2x + h + 3)

Step 4: Apply the limit as h→0h \to 0.

dydx=2x+0+3=2x+3\frac{dy}{dx} = 2x + 0 + 3 = 2x + 3

The derivative is 2x+3\boxed{2x + 3}.

b) y=cos⁡xy = \cos x

Step 1: Write the definition of the derivative from first principles.

dydx=lim⁡h→0f(x+h)−f(x)h\frac{dy}{dx} = \lim_{h \to 0} \frac{f(x+h) - f(x)}{h}

Step 2: Substitute f(x)=cos⁡xf(x) = \cos x and f(x+h)=cos⁡(x+h)f(x+h) = \cos(x+h).

f(x+h)−f(x)=cos⁡(x+h)−cos⁡xf(x+h) - f(x) = \cos(x+h) - \cos x

Step 3: Use the trigonometric identity cos⁡A−cos⁡B=−2sin⁡(A+B2)sin⁡(A−B2)\cos A - \cos B = -2 \sin\left(\frac{A+B}{2}\right) \sin\left(\frac{A-B}{2}\right).

cos⁡(x+h)−cos⁡x=−2sin⁡(2x+h2)sin⁡(h2)=−2sin⁡(x+h2)sin⁡(h2)\cos(x+h) - \cos x = -2 \sin\left(\frac{2x+h}{2}\right) \sin\left(\frac{h}{2}\right) = -2 \sin\left(x + \frac{h}{2}\right) \sin\left(\frac{h}{2}\right)

Step 4: Substitute into the limit and rearrange.

dydx=lim⁡h→0−2sin⁡(x+h2)sin⁡(h2)h=lim⁡h→0[−sin⁡(x+h2)⋅sin⁡(h2)h2]\frac{dy}{dx} = \lim_{h \to 0} \frac{-2 \sin\left(x + \frac{h}{2}\right) \sin\left(\frac{h}{2}\right)}{h} = \lim_{h \to 0} \left[ -\sin\left(x + \frac{h}{2}\right) \cdot \frac{\sin\left(\frac{h}{2}\right)}{\frac{h}{2}} \right]

Step 5: Apply the limit, using lim⁡θ→0sin⁡θθ=1\lim_{\theta \to 0} \frac{\sin \theta}{\theta} = 1.

dydx=−sin⁡(x+0)⋅1=−sin⁡x\frac{dy}{dx} = -\sin(x + 0) \cdot 1 = -\sin x

The derivative is −sin⁡x\boxed{-\sin x}.

3. Find dy/dxdy/dx:

a) y=(x2+1)5y = (x^2 + 1)^5

Step 1: Use the chain rule. Let u=x2+1u = x^2 + 1, so y=u5y = u^5.

Step 2: Differentiate yy with respect to uu and uu with respect to xx.

dydu=5u4\frac{dy}{du} = 5u^4 dudx=2x\frac{du}{dx} = 2x

Step 3: Apply the chain rule dydx=dydu⋅dudx\frac{dy}{dx} = \frac{dy}{du} \cdot \frac{du}{dx}.

dydx=5u4⋅2x=5(x2+1)4⋅2x=10x(x2+1)4\frac{dy}{dx} = 5u^4 \cdot 2x = 5(x^2 + 1)^4 \cdot 2x = 10x(x^2 + 1)^4

The derivative is 10x(x2+1)4\boxed{10x(x^2 + 1)^4}.

b) y=x3e−2xy = x^3 e^{-2x}

Step 1: Use the product rule: ddx(uv)=u′v+uv′\frac{d}{dx}(uv) = u'v + uv'. Let u=x3u = x^3 and v=e−2xv = e^{-2x}.

Step 2: Find the derivatives of uu and vv.

u′=3x2u' = 3x^2 v′=−2e−2xv' = -2e^{-2x}

Step 3: Apply the product rule.

dydx=(3x2)(e−2x)+(x3)(−2e−2x)\frac{dy}{dx} = (3x^2)(e^{-2x}) + (x^3)(-2e^{-2x}) dydx=3x2e−2x−2x3e−2x\frac{dy}{dx} = 3x^2 e^{-2x} - 2x^3 e^{-2x}

Step 4: Factor out common terms.

dydx=x2e−2x(3−2x)\frac{dy}{dx} = x^2 e^{-2x}(3 - 2x)

The derivative is x2e−2x(3−2x)\boxed{x^2 e^{-2x}(3 - 2x)}.

c) y=ln⁡(cos⁡x)y = \ln(\cos x)

Step 1: Use the chain rule. Let u=cos⁡xu = \cos x, so y=ln⁡uy = \ln u.

Step 2: Differentiate yy with respect to uu and uu with respect to xx.

dydu=1u\frac{dy}{du} = \frac{1}{u} dudx=−sin⁡x\frac{du}{dx} = -\sin x

Step 3: Apply the chain rule dydx=dydu⋅dudx\frac{dy}{dx} = \frac{dy}{du} \cdot \frac{du}{dx}.

dydx=1cos⁡x⋅(−sin⁡x)=−sin⁡xcos⁡x=−tan⁡x\frac{dy}{dx} = \frac{1}{\cos x} \cdot (-\sin x) = -\frac{\sin x}{\cos x} = -\tan x

The derivative is −tan⁡x\boxed{-\tan x}.

d) y=arctan⁡(2x)y = \arctan(2x)

Step 1: Use the chain rule. The derivative of arctan⁡u\arctan u is 11+u2dudx\frac{1}{1+u^2} \frac{du}{dx}. Let u=2xu = 2x.

Step 2: Find the derivative of uu with respect to xx.

dudx=2\frac{du}{dx} = 2

Step 3: Apply the chain rule.

dydx=11+(2x)2⋅2=21+4x2\frac{dy}{dx} = \frac{1}{1+(2x)^2} \cdot 2 = \frac{2}{1+4x^2}

The derivative is 21+4x2\boxed{\frac{2}{1+4x^2}}.

e) x2y+y3=5x^2 y + y^3 = 5 (implicit)

Step 1: Differentiate both sides of the equation with respect to xx. Remember to use the product rule for x2yx^2 y and the chain rule for y3y^3.

ddx(x2y)+ddx(y3)=ddx(5)\frac{d}{dx}(x^2 y) + \frac{d}{dx}(y^3) = \frac{d}{dx}(5)

Step 2: Apply differentiation rules.

(2x)y+x2dydx+3y2dydx=0(2x)y + x^2 \frac{dy}{dx} + 3y^2 \frac{dy}{dx} = 0

Step 3: Group terms containing dydx\frac{dy}{dx} and solve for dydx\frac{dy}{dx}.

(x2+3y2)dydx=−2xy(x^2 + 3y^2) \frac{dy}{dx} = -2xy dydx=−2xyx2+3y2\frac{dy}{dx} = \frac{-2xy}{x^2 + 3y^2}

The derivative is −2xyx2+3y2\boxed{\frac{-2xy}{x^2 + 3y^2}}.

f) x=etcos⁡tx = e^t \cos t, y=etsin⁡ty = e^t \sin t (parametric)

Step 1: Use the formula for parametric differentiation: dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}.

Step 2: Find dxdt\frac{dx}{dt} using the product rule.

dxdt=ddt(etcos⁡t)=etcos⁡t+et(−sin⁡t)=et(cos⁡t−sin⁡t)\frac{dx}{dt} = \frac{d}{dt}(e^t \cos t) = e^t \cos t + e^t (-\sin t) = e^t(\cos t - \sin t)

Step 3: Find dydt\frac{dy}{dt} using the product rule.

dydt=ddt(etsin⁡t)=etsin⁡t+etcos⁡t=et(sin⁡t+cos⁡t)\frac{dy}{dt} = \frac{d}{dt}(e^t \sin t) = e^t \sin t + e^t \cos t = e^t(\sin t + \cos t)

Step 4: Substitute into the formula for dydx\frac{dy}{dx}.

dydx=et(sin⁡t+cos⁡t)et(cos⁡t−sin⁡t)\frac{dy}{dx} = \frac{e^t(\sin t + \cos t)}{e^t(\cos t - \sin t)}

Step 5: Simplify by canceling ete^t.

dydx=sin⁡t+cos⁡tcos⁡t−sin⁡t\frac{dy}{dx} = \frac{\sin t + \cos t}{\cos t - \sin t}

The derivative is sin⁡t+cos⁡tcos⁡t−sin⁡t\boxed{\frac{\sin t + \cos t}{\cos t - \sin t}}.

4. Find and classify all stationary points of y=2r3−9r2+12r−3y = 2r^3 - 9r^2 + 12r - 3.

Step 1: Find the first derivative, dydr\frac{dy}{dr}.

dydr=6r2−18r+12\frac{dy}{dr} = 6r^2 - 18r + 12

Step 2: Set the first derivative to zero to find critical points.

6r2−18r+12=06r^2 - 18r + 12 = 0

Divide by 6:

r2−3r+2=0r^2 - 3r + 2 = 0

Factor the quadratic equation:

(r−1)(r−2)=0(r-1)(r-2) = 0

The critical points are r=1r=1 and r=2r=2.

Step 3: Find the corresponding yy values for these critical points.
For r=1r=1: y=2(1)3−9(1)2+12(1)−3=2−9+12−3=2y = 2(1)^3 - 9(1)^2 + 12(1) - 3 = 2 - 9 + 12 - 3 = 2. Point: (1,2)(1, 2).
For r=2r=2: y=2(2)3−9(2)2+12(2)−3=16−36+24−3=1y = 2(2)^3 - 9(2)^2 + 12(2) - 3 = 16 - 36 + 24 - 3 = 1. Point: (2,1)(2, 1).

Step 4: Find the second derivative, d2ydr2\frac{d^2y}{dr^2}, to classify the stationary points.

d2ydr2=12r−18\frac{d^2y}{dr^2} = 12r - 18

Step 5: Evaluate the second derivative at each critical point.
For r=1r=1: d2ydr2=12(1)−18=−6\frac{d^2y}{dr^2} = 12(1) - 18 = -6. Since −6<0-6 < 0, (1,2)(1, 2) is a local maximum.
For r=2r=2: d2ydr2=12(2)−18=6\frac{d^2y}{dr^2} = 12(2) - 18 = 6. Since 6>06 > 0, (2,1)(2, 1) is a local minimum.

The stationary points are:

  • (1,2)(1, 2), which is a local maximum.
  • (2,1)(2, 1), which is a local minimum.

5. A rectangular box with no lid has a square base of side xx and height hh. Given that the total surface area is 75 cm275 \text{ cm}^2, find the dimensions for maximum volume.

Step 1: Write expressions for the volume (VV) and surface area (AA).
Volume: V=x2hV = x^2 h
Surface Area (base + 4 sides): A=x2+4xhA = x^2 + 4xh

Step 2: Use the given surface area (A=75 cm2A=75 \text{ cm}^2) to express hh in terms of xx.

75=x2+4xh  ⟹  4xh=75−x2  ⟹  h=75−x24x75 = x^2 + 4xh \implies 4xh = 75 - x^2 \implies h = \frac{75 - x^2}{4x}

Step 3: Substitute hh into the volume equation to get V(x)V(x).

V(x)=x2(75−x24x)=x(75−x2)4=75x−x34=754x−14x3V(x) = x^2 \left(\frac{75 - x^2}{4x}\right) = \frac{x(75 - x^2)}{4} = \frac{75x - x^3}{4} = \frac{75}{4}x - \frac{1}{4}x^3

Step 4: Find the first derivative of V(x)V(x) and set it to zero to find critical points.

dVdx=754−34x2\frac{dV}{dx} = \frac{75}{4} - \frac{3}{4}x^2 754−34x2=0  ⟹  75−3x2=0  ⟹  3x2=75  ⟹  x2=25\frac{75}{4} - \frac{3}{4}x^2 = 0 \implies 75 - 3x^2 = 0 \implies 3x^2 = 75 \implies x^2 = 25

Since xx must be positive, x=5 cmx = 5 \text{ cm}.

Step 5: Find the corresponding height hh.

h=75−(5)24(5)=75−2520=5020=2.5 cmh = \frac{75 - (5)^2}{4(5)} = \frac{75 - 25}{20} = \frac{50}{20} = 2.5 \text{ cm}

Step 6: Use the second derivative test to confirm it's a maximum.

d2Vdx2=−64x=−32x\frac{d^2V}{dx^2} = -\frac{6}{4}x = -\frac{3}{2}x

At x=5x=5: d2Vdx2=−32(5)=−152\frac{d^2V}{dx^2} = -\frac{3}{2}(5) = -\frac{15}{2}. Since this is negative, it's a maximum.

The dimensions for maximum volume are x=5 cmx = \boxed{5 \text{ cm}} and h=2.5 cmh = \boxed{2.5 \text{ cm}}.

6. Water leaks from a conical tank (vertex down) at 3 m3/min3 \text{ m}^3/\text{min}. The tank has radius 2 m2 \text{ m} and height 5 m5 \text{ m}. Find the rate at which the water level falls when the depth is 3 m3 \text{ m}.

Step 1: Identify given information and what to find.
Given: dVdt=−3 m3/min\frac{dV}{dt} = -3 \text{ m}^3/\text{min} (negative because water is leaking).
Tank dimensions: R=2 mR = 2 \text{ m}, H=5 mH = 5 \text{ m}.
Find: dhdt\frac{dh}{dt} when h=3 mh = 3 \text{ m}.

Step 2: Write the volume of a cone: V=13πr2hV = \frac{1}{3}\pi r^2 h.

Step 3: Use similar triangles to relate rr and hh for the water in the cone.

rh=RH=25  ⟹  r=25h\frac{r}{h} = \frac{R}{H} = \frac{2}{5} \implies r = \frac{2}{5}h

Step 4: Substitute rr into the volume formula to express VV in terms of hh.

V=13π(25h)2h=13π(425h2)h=4π75h3V = \frac{1}{3}\pi \left(\frac{2}{5}h\right)^2 h = \frac{1}{3}\pi \left(\frac{4}{25}h^2\right) h = \frac{4\pi}{75}h^3

Step 5: Differentiate VV with respect to time tt.

dVdt=4π75⋅3h2dhdt=4π25h2dhdt\frac{dV}{dt} = \frac{4\pi}{75} \cdot 3h^2 \frac{dh}{dt} = \frac{4\pi}{25}h^2 \frac{dh}{dt}

Step 6: Substitute the known values (dVdt=−3\frac{dV}{dt} = -3, h=3h=3) and solve for dhdt\frac{dh}{dt}.

−3=4π25(3)2dhdt-3 = \frac{4\pi}{25}(3)^2 \frac{dh}{dt}
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