Tangent to a cycloid

Find the tangent line (described parametrically) to the cycloid (4t−4sin⁡t,4−4cos⁡t) when t=π/4.

Solution

(1) Compute x′ and y′.

Find x′(t) and y′(t):

x(t)=4t−4sin⁡t≫≫x′(t)=4−4cos⁡ty(t)=4−4cos⁡t≫≫y′(t)=4sin⁡t

(2) Plug in t=π/4:

x′(π/4)≫≫4−4cos⁡(π/4)≫≫4−22y′(π/4)≫≫4sin⁡(π/4)≫≫22

(3) Apply formula: dydx=y′x′:

Calculate dydx at t=π/4:

dydx(π/4)=y′(π/4)x′(π/4)≫≫224−22≫≫224−22⋅4+224+22≫≫82+816−8≫≫2+1

So:

dydx|t=π/4=2+1

This is the slope m for our line.


(4) Need the point P for our line. Find (x,y) at t=π/4.

Plug t=π/4 into parametric formulas:

(x(t),y(t))|t=π/4≫≫(4π4−4sin⁡(π/4),4−4cos⁡(π/4))≫≫(π−22,4−22)

(5) Point-slope formulation of tangent line:

x=a+t,y=b+mt

Inserting data:

x=(π−22)+t,y=(4−22)+(2+1)t

Vertical and horizontal tangents of the circle

Consider the circle parametrized by x=cos⁡t and y=sin⁡t. Find the points where the tangent lines are vertical or horizontal.

Solution

(1) For the points with vertical tangent line, we find where the moving point has x′(t)=0 (purely vertical motion):

x′(t)=−sin⁡t,x′(t)=0≫≫−sin⁡t=0≫≫t=0,π

The moving point is at (1,0) when t=0, and at (−1,0) when t=π.


(2) For the points with horizontal tangent line, we find where the moving point has y′(t)=0 (purely horizontal motion):

y′(t)=cos⁡t,y′(t)=0≫≫cos⁡t=0≫≫t=π2,3π2

The moving point is at (0,1) when t=π/2, and at (0,−1) when t=3π/2.

Finding the point with specified slope

Consider the parametric curve given by (x,y)=(t2,t3). Find the point where the slope of the tangent line to this curve equals 5.

Solution

(1) Compute the derivatives:

x′(t)=2t,y′(t)=3t2

Therefore the slope of the tangent line, in terms of t:

m=dydx=y′(t)x′(t)≫≫3t22t≫≫32t

(2) Set up equation:

m=532t=5≫≫t=103

(3) Find the point:

(x,y)|t=10/3≫≫(1009,100027)

Perimeter of a circle

(1) The perimeter of the circle (Rcos⁡t,Rsin⁡t) is easily found. We have (x′,y′)=(−Rsin⁡t,Rcos⁡t), and therefore:

(x′)2+(y′)2=(−Rsin⁡t)2+(Rcos⁡t)2≫≫R2sin2⁡t+R2cos2⁡t≫≫R2ds=(x′)2+(y′)2dt=Rdt

(2) Integrate around the circle:

Perimeter=∫02πds≫≫∫02πRdt≫≫Rt|02π=2πR

Perimeter of an asteroid

Find the perimeter length of the ‘asteroid’ given parametrically by (x,y)=(acos3⁡θ,asin3⁡θ) for a=2.

Solution

(1) Notice: Throughout this problem we use the parameter θ instead of t. This does not mean we are using polar coordinates!

Compute the derivatives in θ:

(x′,y′)=(3acos2⁡θsin⁡θ,3asin2⁡θcos⁡θ)

(2) Compute the infinitesimal arc element.

(x′)2+(y′)2≫≫9a2cos4⁡θsin2⁡θ+9a2sin4⁡θcos2⁡θ≫≫9a2sin2⁡θcos2⁡θ(cos2⁡θ+sin2⁡θ)≫≫9a2sin2⁡θcos2⁡θ

Plug into the arc element, simplify:

ds=(x′)2+y′)2dθ≫≫9a2sin2⁡θcos2⁡θdθ≫≫ds=3a|sin⁡θcos⁡θ|dθ

(3) Bounds of integration?

Easiest to use θ∈[0,π/2]. This covers one edge of the asteroid. Then multiply by 4 for the final answer.

On the interval θ∈[0,π/2], the factor 3asin⁡θcos⁡θ is positive. So we can drop the absolute value and integrate directly.

Absolute values matter!

If we tried to integrate on the whole range θ∈[0,2π], then 3asin⁡θcos⁡θ really does change sign.

To perform integration properly with these absolute values, we’d need to convert to a piecewise function by adding appropriate minus signs.


(4) Integrate the arc element:

∫0π/2ds≫≫∫0π/23asin⁡θcos⁡θdθ≫≫3a∫u=01udu(u=sin⁡θ)≫≫3au22|01≫≫3a2

Finally, multiply by 4 to get the total perimeter: L=6a

Speed, distance, displacement

The parametric curve (t,23t3/2) describes the position of a moving particle (t measuring seconds). (a) What is the speed function?

Suppose the particle travels for 8 seconds starting at t=0. (b) What is the total distance traveled? (c) What is the total displacement?

Solution

(a)

Compute derivatives:

(x′,y′)=(1,t1/2)

Now compute the speed:

(x′)2+(y′)2=1+(t1/2)2=1+t≫≫v(t)=(x′)2+(y′)2=1+t

(b)

Distance traveled by using speed.

Compute total distance traveled function:

s(t)=∫u=0t1+udu

Substitute w=1+u and dw=du. New bounds are 1 and 1+t. Calculate:

≫≫∫11+twdw≫≫23w3/2|11+t≫≫23((1+t)3/2−1)

The distance traveled up to t=8 is:

s(8)=23(93/2−1)≫≫23(27−1)≫≫523

(c)

Displacement formula: d=(x1−x0)2+(y1−y0)2

Now compute starting and ending points.

For starting point, insert t=0:

(x(t),y(t))|t=0≫≫(t,23t3/2)|t=0≫≫(0,0)

For ending point, insert t=8:

(x(t),y(t))|t=8≫≫(t,23t3/2)|t=8≫≫(8,2383/2)≫≫(8,3223)

Insert (0,0) and (8,322/3):

≫≫82+(3223)2≫≫64+20489≫≫26243

Surface of revolution - parametric circle

By revolving the unit upper semicircle about the x-axis, we can compute the surface area of the unit sphere.

Parametrization of the unit upper semicircle:

(x,y)=(cos⁡t,sin⁡t)≫≫(x′,y′)=(−sin⁡t,cos⁡t)

Therefore, the arc element:

ds=(x′)2+(y′)2dt≫≫(−sin⁡t)2+(cos⁡t)2dt≫≫dt

Now for R(t) we choose R(t)=y(t)=sin⁡t because we are revolving about the x-axis.


Plugging all this into the integral formula and evaluating gives:

A=∫0π2πsin⁡tdt≫≫−2πcos⁡t|0π≫≫4π

Notice: This method is a little easier than the method using the graph y=1−x2.

Surface of revolution - parametric curve

Set up the integral which computes the surface area of the surface generated by revolving about the x-axis the curve (t3,t2−1) for 0≤t≤1.

Solution

For revolution about the x-axis, we set R=y(t)=t2−1.

Then compute ds:

ds=(x′)2+(y′)2≫≫(3t2)2+(2t)2≫≫9t4+4t2≫≫t2(9t2+4)≫≫t9t2+4

Therefore the desired integral is:

A=∫012πRds≫≫∫012π(t2−1)t9t2+4dt