Problem 28
Question
Let $$f(x, y)=2 x^{3}-3 y x$$ Compute \(f_{x}(1,2)\) and \(f_{y}(1,2)\), and interpret these partial derivatives geometrically.
Step-by-Step Solution
Verified Answer
\(f_x(1,2) = 0\); \(f_y(1,2) = -3\). The function is flat in the x-direction and decreases in the y-direction at (1, 2).
1Step 1: Partial Derivative with Respect to x
To find the partial derivative of the function with respect to \(x\), we treat \(y\) as a constant and differentiate. Given: \[f(x, y) = 2x^3 - 3yx\]The partial derivative \(f_x\) is:\[\frac{\partial f}{\partial x} = \frac{\partial}{\partial x}(2x^3 - 3yx)\]Applying the derivative rules, we get:\[\frac{\partial f}{\partial x} = 6x^2 - 3y\]Now substituting \(x = 1\) and \(y = 2\):\[f_x(1,2) = 6(1)^2 - 3(2) = 6 - 6 = 0\]
2Step 2: Partial Derivative with Respect to y
To find the partial derivative with respect to \(y\), treat \(x\) as constant.Given:\[f(x, y) = 2x^3 - 3yx\]The partial derivative \(f_y\) is:\[\frac{\partial f}{\partial y} = \frac{\partial}{\partial y}(2x^3 - 3yx)\]The only term involving \(y\) is \(-3yx\), so:\[\frac{\partial f}{\partial y} = -3x\]Substitute \(x = 1\) into the equation:\[f_y(1,2) = -3(1) = -3\]
3Step 3: Geometrical Interpretation of Partial Derivatives
The partial derivative \(f_x(1,2) = 0\) indicates that at the point \((1, 2)\), the rate of change of the function along the x-direction is zero. This means the tangent line to the surface at this point is flat along the x-axis.The partial derivative \(f_y(1,2) = -3\) suggests that the function decreases at a rate of 3 units in the y-direction. Thus, the surface slopes downwards in the y-direction at this point.
Key Concepts
Geometrical Interpretation of Partial DerivativesRate of Change in Multi-Variable FunctionsDifferentiation Rules for Calculating Partial Derivatives
Geometrical Interpretation of Partial Derivatives
Visualizing how functions behave in a multi-dimensional space involves considering surfaces. When we calculate partial derivatives, we look at how the surface defined by a function changes as we move a little in one direction while keeping the other direction constant. In simple terms, partial derivatives tell us the slope of the curve we get if we slice through the surface along a coordinate axis.
For the function given, when we compute the partial derivative with respect to \(x\) at a specific point, it shows how steeply the surface rises or falls as we move just a tiny bit in the \(x\)-direction. Specifically in our problem, \(f_x(1,2) = 0\) shows that at point \((1,2)\), movement along the \(x\)-axis doesn't change the function's value; the surface is flat in this direction.
For the function given, when we compute the partial derivative with respect to \(x\) at a specific point, it shows how steeply the surface rises or falls as we move just a tiny bit in the \(x\)-direction. Specifically in our problem, \(f_x(1,2) = 0\) shows that at point \((1,2)\), movement along the \(x\)-axis doesn't change the function's value; the surface is flat in this direction.
- Flat surface in the direction of the \(x\)-axis at point \((1, 2)\).
- Downward slope in the \(y\)-direction at point \((1, 2)\).
Rate of Change in Multi-Variable Functions
In mathematics, the concept of rate of change is crucial for understanding how a function's output behaves in response to varying its inputs. Particularly, in multi-variable functions, partial derivatives represent these rates of changes.
When you take the partial derivative with respect to a particular variable, you're essentially zooming in on how changing just that one variable alters the function when all other variables are kept constant. Imagine you are probing a multi-dimensional surface for inclines.
In the context of this exercise, when we calculate \(f_x(1,2) = 0\), it signifies that infinitesimal shifts in the \(x\)-value while \(y\) is fixed do not change the function's value at that spot. It's like standing on level ground, where a step forward won't change your height.
When you take the partial derivative with respect to a particular variable, you're essentially zooming in on how changing just that one variable alters the function when all other variables are kept constant. Imagine you are probing a multi-dimensional surface for inclines.
In the context of this exercise, when we calculate \(f_x(1,2) = 0\), it signifies that infinitesimal shifts in the \(x\)-value while \(y\) is fixed do not change the function's value at that spot. It's like standing on level ground, where a step forward won't change your height.
- \(f_x(1,2) = 0\) implies no change along the \(x\) direction.
- \(f_y(1,2) = -3\) represents {change by 3 units decrease/increase in \(f\) for unit movement in \(y\).
Differentiation Rules for Calculating Partial Derivatives
Calculating partial derivatives is an application of differentiation, but with a special focus on multi-variable functions. To compute these derivatives, we adhere to foundational differentiation rules, modifying them slightly due to the presence of several variables.
Let's delve into the differentiation rules used in calculating the partial derivatives in the given exercise:
By using these rules consistently, we simplify the process of understanding how each variable uniquely influences the function. Hence, differentiation rules act like lenses through which we can distinctly see each component's effect on the function's geometry and behavior.
Let's delve into the differentiation rules used in calculating the partial derivatives in the given exercise:
- Product Rule: It's important when dealing with multi-variable functions, especially when variables are multiplied together. However, in this exercise, simplification is straightforward as each differentiation is carried out while considering one variable constant.
- Constant Rule: When differentiating with respect to one variable, treat the other variables as constants. This simplification outlines the difference between single and partial derivatives.
By using these rules consistently, we simplify the process of understanding how each variable uniquely influences the function. Hence, differentiation rules act like lenses through which we can distinctly see each component's effect on the function's geometry and behavior.
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