1 Part 1: Traces
The cone and paraboloid are two mathematical surfaces with distinct shapes that, at first glance, may appear to be similar. A cursory examination of both Figure 1 and Figure 2 reveals that both shapes exhibit an almost circular-like distribution. However, upon delving deeper into this project, I will demonstrate how significantly different these shapes are.
Upon observing the contour maps of the cone and paraboloid, a notable disparity in their growth patterns is immediately discernible. Specifically, the paraboloid exhibits a rate of growth that could be described as approaching an exponential function, evidenced by the discrepancy in growth between z = 4 and z = 3 when compared to the difference in growth between z = 2 and z = 3.
In contrast, the growth of the cone appears to be more uniform across its di- mensions. This observation could be attributed to the paraboloidβs underlying quadratic equation, which imparts a degree of curvature and accentuates the
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rate of growth in the z direction. Such distinctions are critical to understand- ing the properties and applications of these shapes in various fields, including physics, engineering, and mathematics.
2 Part 2: Directional Derivatives
I began by calculating the directional derivatives and magnitude of both shapes:
2.1 Step 1
Find the Gradient Vector and Magnitude for z = x2 + y2: RecalltheGradientVectorFormula: βf=τ°fx,fy,fzτ°=βfi+βfj+βfk
βx βy βz
βf =2x, βf =2y, βf =β1βββf =τ°2x,2y,β1τ° βx βy βz
Plugging in the point (1, 0, 1), we have: βf(1,0,1) = τ°2,0,β1τ°
Gradient Vector: τ°2,0,β1τ° τ°τ°τ°τ°τ° β
τ° 2,0,β1 τ°= 22 +02 +(β1)2 = 5 β
Magnitude: = 5
2.2 Step 2
Find the Gradient Vector and Magnitude for z = τ°x2 + y2: RecalltheGradientVectorFormula: βf=τ°fx,fy,fzτ°=βfi+βfj+βfk
βx βy βz
βf x βf y βf τ° x y τ° βx = τ°x2 +y2, βy = τ°x2 +y2, βz =β1βββf = τ°x2 +y2,τ°x2 +y2,β1
Plugging in the point (1, 0, 1), we have:
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2.3 Final Answer
βf(1,0,1) = τ°1,0,β1τ° Gradient Vector: τ°1,0,β1τ°
τ°τ°τ°τ°τ° β τ° 1,0,β1 τ°= 12 +02 +(β1)2 = 2
β
Magnitude: = 2
Upon analyzing the rate of change of the surface areas of a paraboloid and a cone, it is evident that the paraboloid has the highest rate of increase, with a
ββ
value of 5, while the cone has a rate of increase of 2. The computation of the greatest increase highlights the substantial difference between the two shapes, revealing that the paraboloid increases at a much faster rate than the cone.
Furthermore, observing the contour maps for both shapes provides a graph- ical representation of their rate of change. From the contour map, it is clear that the paraboloid has a much larger increase as compared to the cone, while the latter seems to increase at a relatively constant rate.
3 Part 3: Tangent Places
Suppose that f has a continuous partial deriva- tive. An equation of the tangent plane to the surface. An equation of the tangent plane to the surface z = f(x,y) at the point P(x0,y0,z0) is given by:
β f τ°τ° τ°τ° β f τ°τ° τ°τ°
zβz0 = βxτ°(x0,y0)(xβx0)τ°+ βyτ°(x0,y0)(yβy0)τ° τ°τ°τ°τ°
3.1 Step 1
Find the Tangent Planes on P (0, 0, 0) for z = x2 + y2 βf =2x, βf =2y,
βx βy Plugging in x = 0 and y = 0, we get:
z β 0 = 2x(0, 0)(x β 0) + 2y(0, 0)(y β 0) 3
so the equation of the tangent plane is:
z=0
3.2 Step 2
βx=τ°x2+y2, βy=τ°x2+y2, Plugging in x = 0 and y = 0, we get:
xy
z β 0 = τ°x2 + y2 (0, 0)(x β 0) + τ°x2 + y2 (0, 0)(y β 0)
so the equation of the tangent plane is:
z = 0.
3.3 Step 3
Plotting the surface and the tangent
3DimageofbothZ=τ°x2+y2 andZ=x2+y2
To provide a comprehensive understanding of the cone and paraboloid shapes, I decided to utilize the powerful visualization tool, GeoGebra 3D. This tool al- lows for an interactive 3D representation of the shapes, which provides a better insight into their structure and properties.
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Find the Tangent Planes on P (0, 0, 0) for Z = τ°x2 + y2 βf x βf y
3.4 Final Answer
Therefore, in our effort to derive the equation of the tangent plane to the surface z = f(x,y) at the point P(0,0,0), we have obtained z = 0 as the equation of the tangent plane. This result indicates that the tangent line at the origin lies on the x-y plane. This finding can also be clearly observed in the accompanying graphs (figure 1 & 2), where the point P (0, 0, 0) is seen to be untouched by the surface.
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