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  1. passes through (a,b). Why? If you travel on a level curve, the value of f does not change. And the instantaneous direction of motion at any point on this curve is the tangent vector to the curve at that point. 2. The gradient vector ~∇ f(a,b) must be perpendicular to the level curve of f that passes through (a,b). These results are sketched ...

  2. Level Curves and Contour Plots. Level curves and contour plots are another way of visualizing functions of two variables. If you have seen a topographic map then you have seen a contour plot. Example: To illustrate this we first draw the graph of z = x2 + y2. On this graph we draw contours, which are curves at a fixed height z = constant.

  3. Motion on a Curve => The net force on a car traveling around a curve is the centripetal force, F c = m v 2 / r, directed toward the center of the curve. => For a level curve, the centripetal force will be supplied by the friction force between the tires and roadway.

  4. Level Curves and Surfaces. A level curve, or surface, is a set on which f is constant. If you are on a level curve, and you want to stay on that curve, which way should you travel? Using the mountain analogy, determine the direction of maximum slope and turn 90°. This takes you neither up hill nor down hill, but along the side of the mountain.

  5. 15.5.4 The Gradient and Level Curves. Recall from Section 15.1 that the curve. is a constant, is a level curve, on which function values are constant. Combining these two observations, we conclude that the gradient. Let. We now differentiate. The derivative of the right side is 0.

  6. The range of g g is the closed interval [0, 3] [0, 3]. First, we choose any number in this closed interval—say, c =2 c = 2. The level curve corresponding to c = 2 c = 2 is described by the equation. √9−x2 −y2 = 2 9 − x 2 − y 2 = 2. To simplify, square both sides of this equation: 9−x2 −y2 = 4 9 − x 2 − y 2 = 4.

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  8. Feb 24, 2024 · In the merry-go-round’s frame of reference, we explain the apparent curve to the right by using an inertial force, called the Coriolis force, which causes the ball to curve to the right. The Coriolis force can be used by anyone in that frame of reference to explain why objects follow curved paths and allows us to apply Newton’s laws in noninertial frames of reference.

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