The Central Idea
Suppose
\[ z=f(x,y). \]The output \(z\) may change when \(x\) changes, when \(y\) changes, or when both change.
A partial derivative asks what happens when we change only one input at a time.
To differentiate with respect to \(x\), treat \(y\) as a constant. To differentiate with respect to \(y\), treat \(x\) as a constant.
From One Variable to Several Variables
In one-variable calculus,
\[ y=f(x) \]has one input direction, so the derivative
\[ f'(x) \]measures the local rate of change along that direction.
For
\[ z=f(x,y), \]there are at least two independent input directions, so we need separate derivatives for those directions.
The Partial Derivative with Respect to \(x\)
The partial derivative of \(f\) with respect to \(x\) is written
\[ \boxed{f_x(x,y)} \]or
\[ \boxed{\frac{\partial f}{\partial x}}. \]It measures how \(f\) changes as \(x\) changes while \(y\) is held fixed.
The Partial Derivative with Respect to \(y\)
The partial derivative with respect to \(y\) is written
\[ \boxed{f_y(x,y)} \]or
\[ \boxed{\frac{\partial f}{\partial y}}. \]It measures how \(f\) changes as \(y\) changes while \(x\) is held fixed.
Why the Symbol \(\partial\) Appears
Ordinary derivatives often use
\[ \frac{dy}{dx}. \]Partial derivatives use the rounded symbol
\[ \partial \]to emphasize that we are measuring only one part of a multivariable dependence.
Thus,
\[ \frac{\partial z}{\partial x} \]means the partial change of \(z\) with respect to \(x\).
Operational Rule
To compute
\[ \frac{\partial f}{\partial x}, \]treat every variable other than \(x\) as a constant.
To compute
\[ \frac{\partial f}{\partial y}, \]treat every variable other than \(y\) as a constant.
This is the main computational habit of partial differentiation.
Example: A Simple Polynomial
Let
\[ f(x,y)=x^2+3y. \]Differentiate with respect to \(x\). Since \(y\) is treated as constant,
\[ f_x(x,y)=2x. \]Differentiate with respect to \(y\). Since \(x\) is treated as constant,
\[ f_y(x,y)=3. \]Therefore,
\[ \boxed{f_x=2x,\qquad f_y=3}. \]Example: Products of Variables
Consider
\[ f(x,y)=x^2y^3. \]With respect to \(x\), \(y^3\) behaves like a constant coefficient:
\[ f_x=2xy^3. \]With respect to \(y\), \(x^2\) behaves like a constant coefficient:
\[ f_y=3x^2y^2. \]Thus,
\[ \boxed{f_x=2xy^3,\qquad f_y=3x^2y^2}. \]Terms Independent of the Active Variable Disappear
Suppose
\[ f(x,y)=4x^3-7y^2+5. \]When differentiating with respect to \(x\), both \(-7y^2\) and \(5\) are constants:
\[ f_x=12x^2. \]When differentiating with respect to \(y\), both \(4x^3\) and \(5\) are constants:
\[ f_y=-14y. \]Example: Several Terms
Let
\[ f(x,y)=3x^4y^2-5x^2y+7y^3-9. \]With respect to \(x\),
\[ \boxed{f_x=12x^3y^2-10xy}. \]With respect to \(y\),
\[ \boxed{f_y=6x^4y-5x^2+21y^2}. \]Partial Derivatives Are Functions
A partial derivative is usually not just one number. It is another function.
If
\[ f(x,y)=x^2y+y^2, \]then
\[ f_x(x,y)=2xy \]and
\[ f_y(x,y)=x^2+2y. \]These functions tell us the \(x\)- and \(y\)-rates of change at every point where the derivatives exist.
Evaluating a Partial Derivative at a Point
Suppose
\[ f(x,y)=x^2y+y^2. \]We found
\[ f_x=2xy. \]At the point \((2,3)\),
\[ f_x(2,3)=2(2)(3)=12. \]So at \((2,3)\), the function changes at an instantaneous rate of \(12\) units of output per unit increase in \(x\), with \(y\) held fixed.
Evaluating the Other Direction
For the same function,
\[ f_y=x^2+2y. \]At \((2,3)\),
\[ f_y(2,3)=2^2+2(3)=10. \]The local rate in the \(y\)-direction is therefore \(10\).
Limit Definition of a Partial Derivative
The partial derivative with respect to \(x\) can be defined by
\[ \boxed{ f_x(a,b) = \lim_{h\to0} \frac{f(a+h,b)-f(a,b)}{h} }. \]Notice that only the first coordinate changes.
Similarly,
\[ \boxed{ f_y(a,b) = \lim_{h\to0} \frac{f(a,b+h)-f(a,b)}{h} }. \]Here only the second coordinate changes.
Partial Derivatives Are Ordinary Derivatives Along Slices
Fix \(y=b\). Then
\[ g(x)=f(x,b) \]is an ordinary one-variable function.
Its derivative is
\[ g'(a)=f_x(a,b). \]Likewise, fixing \(x=a\) gives
\[ h(y)=f(a,y), \]with
\[ h'(b)=f_y(a,b). \]Geometric Meaning
For a surface
\[ z=f(x,y), \]fixing \(y=b\) slices the surface with the vertical plane \(y=b\).
The slope of that cross-sectional curve at \((a,b,f(a,b))\) is
\[ f_x(a,b). \]Similarly, fixing \(x=a\) produces a cross section whose slope is
\[ f_y(a,b). \]Two Coordinate Slopes at One Point
A surface generally has more than one meaningful slope at a point.
At \((a,b)\),
\[ f_x(a,b) \]measures slope in the positive \(x\)-direction, while
\[ f_y(a,b) \]measures slope in the positive \(y\)-direction.
Later, directional derivatives will extend this idea to arbitrary directions.
Example: A Paraboloid
Let
\[ f(x,y)=x^2+y^2. \]Then
\[ f_x=2x,\qquad f_y=2y. \]At \((1,2)\),
\[ f_x(1,2)=2 \]and
\[ f_y(1,2)=4. \]The surface rises more rapidly in the positive \(y\)-direction than in the positive \(x\)-direction at that point.
Partial Derivatives with Exponentials
Consider
\[ f(x,y)=e^{xy}. \]With respect to \(x\), use the chain rule:
\[ f_x=ye^{xy}. \]With respect to \(y\),
\[ f_y=xe^{xy}. \]Therefore,
\[ \boxed{f_x=ye^{xy},\qquad f_y=xe^{xy}}. \]Partial Derivatives with Logarithms
Let
\[ f(x,y)=\ln(x^2+y^2). \]Using the chain rule,
\[ f_x= \frac{2x}{x^2+y^2}, \]and
\[ f_y= \frac{2y}{x^2+y^2}. \]These formulas are valid where
\[ x^2+y^2>0. \]Partial Derivatives with Trigonometric Functions
Consider
\[ f(x,y)=\sin(xy)+\cos y. \]With respect to \(x\),
\[ f_x=y\cos(xy). \]With respect to \(y\),
\[ f_y=x\cos(xy)-\sin y. \]Product Rule in Partial Differentiation
The ordinary derivative rules still apply.
If
\[ f(x,y)=x^2e^y, \]then with respect to \(x\),
\[ f_x=2xe^y, \]because \(e^y\) is constant with respect to \(x\).
With respect to \(y\),
\[ f_y=x^2e^y. \]When the Product Rule Is Actually Needed
Consider
\[ f(x,y)=x\sin(xy). \]With respect to \(x\), both factors depend on \(x\), so the product rule is needed:
\[ f_x = \sin(xy)+xy\cos(xy). \]With respect to \(y\), the factor \(x\) is constant:
\[ f_y=x^2\cos(xy). \]Quotient Rule in Partial Differentiation
Let
\[ f(x,y)=\frac{x+y}{x-y}. \]With respect to \(x\),
\[ f_x = \frac{(1)(x-y)-(x+y)(1)}{(x-y)^2} = \frac{-2y}{(x-y)^2}. \]With respect to \(y\),
\[ f_y = \frac{(1)(x-y)-(x+y)(-1)}{(x-y)^2} = \frac{2x}{(x-y)^2}. \]Chain Rule in Partial Differentiation
If
\[ f(x,y)=\sqrt{1+x^2+y^2}, \]then
\[ f_x = \frac{x}{\sqrt{1+x^2+y^2}} \]and
\[ f_y = \frac{y}{\sqrt{1+x^2+y^2}}. \]The same chain-rule logic from one-variable calculus applies separately in each active variable.
Functions of Three Variables
Partial differentiation extends directly to more inputs.
If
\[ w=f(x,y,z), \]then the first partial derivatives are
\[ f_x,\qquad f_y,\qquad f_z. \]Each one varies one coordinate while holding the other two fixed.
Example: Three Variables
Let
\[ f(x,y,z)=x^2yz^3+4xy-z. \]Then
\[ \boxed{f_x=2xyz^3+4y}, \] \[ \boxed{f_y=x^2z^3+4x}, \]and
\[ \boxed{f_z=3x^2yz^2-1}. \]First-Order Partial Derivatives
The derivatives
\[ f_x,\qquad f_y \]are called first-order partial derivatives.
They measure first-order sensitivity of the output to each coordinate direction.
Second-Order Partial Derivatives
Partial derivatives can themselves be differentiated.
Starting from
\[ f_x, \]we may differentiate again with respect to \(x\):
\[ f_{xx}. \]Or we may differentiate \(f_x\) with respect to \(y\):
\[ f_{xy}. \]The Four Second Partials in Two Variables
For a sufficiently differentiable function \(f(x,y)\), the four standard second-order partial derivatives are
\[ \boxed{ f_{xx},\qquad f_{xy},\qquad f_{yx},\qquad f_{yy} }. \]The repeated-index derivatives \(f_{xx}\) and \(f_{yy}\) are called pure second partials.
The derivatives \(f_{xy}\) and \(f_{yx}\) are called mixed partials.
Notation for Second Partials
Common equivalent notations include
\[ f_{xx} = \frac{\partial^2 f}{\partial x^2}, \] \[ f_{yy} = \frac{\partial^2 f}{\partial y^2}, \]and
\[ f_{xy} = \frac{\partial}{\partial y} \left( \frac{\partial f}{\partial x} \right). \]Example: Second Partials
Let
\[ f(x,y)=x^3y^2+2xy. \]First derivatives:
\[ f_x=3x^2y^2+2y, \] \[ f_y=2x^3y+2x. \]Second derivatives:
\[ f_{xx}=6xy^2, \] \[ f_{xy}=6x^2y+2, \] \[ f_{yx}=6x^2y+2, \] \[ f_{yy}=2x^3. \]Mixed Partials Often Agree
In the previous example,
\[ f_{xy}=f_{yx}. \]For many well-behaved functions, the order of mixed partial differentiation does not matter.
A standard sufficient condition is that the relevant second partial derivatives are continuous near the point.
Clairaut's Theorem
Under standard smoothness conditions,
\[ \boxed{f_{xy}=f_{yx}}. \]This result is commonly called Clairaut's theorem, or the equality of mixed partials.
The equality is extremely useful, but it should not be treated as an automatic identity for every imaginable function.
Second Partials as Curvature Information
The derivative
\[ f_{xx} \]describes how the \(x\)-direction slope itself changes as \(x\) changes.
Likewise,
\[ f_{yy} \]describes how the \(y\)-direction slope changes as \(y\) changes.
These ideas will later contribute to multivariable curvature and optimization tests.
Mixed Partials as Interaction Information
The mixed partial
\[ f_{xy} \]asks how the \(x\)-direction rate changes when \(y\) changes.
In applied settings, this can measure interaction between inputs.
A nonzero mixed partial indicates that the effect of one input may depend on the level of another.
Example: Economic Interpretation
Suppose
\[ P(x,y) \]represents profit from two production inputs.
Then
\[ P_x \]measures the marginal change in profit when \(x\) increases while \(y\) remains fixed.
Similarly,
\[ P_y \]measures the marginal change associated with \(y\).
Example: Temperature Field
Suppose
\[ T(x,y) \]gives temperature at a location in a flat region.
Then
\[ T_x \]measures the local east-west temperature rate of change if the \(x\)-axis is east-west, while
\[ T_y \]measures the local north-south rate of change.
Example: Height Field
If
\[ h(x,y) \]gives terrain elevation, then
\[ h_x(a,b) \]describes the instantaneous uphill or downhill slope in the \(x\)-direction at \((a,b)\).
The sign tells whether elevation increases or decreases in that direction.
Interpreting the Sign
At a point:
- if \(f_x>0\), increasing \(x\) locally increases \(f\);
- if \(f_x<0\), increasing \(x\) locally decreases \(f\);
- if \(f_x=0\), the instantaneous \(x\)-direction rate is zero.
The same interpretation applies to \(f_y\).
Units of Partial Derivatives
Partial derivatives carry units.
If \(f\) is measured in dollars and \(x\) is measured in units of product, then
\[ f_x \]has units
\[ \frac{\text{dollars}}{\text{unit of product}}. \]Dimensional interpretation remains just as important in multivariable calculus as in one-variable calculus.
Holding Other Variables Fixed Is a Modeling Assumption
The phrase “hold the other variables fixed” is mathematically precise but may represent an idealized experiment in an application.
Real variables can be physically linked. A partial derivative isolates one coordinate effect even when a real system may later require a more complete coupled analysis.
Partial Derivatives and Level Curves
The previous lesson introduced level curves
\[ f(x,y)=c. \]Partial derivatives describe how the function changes as we cross through those levels along the coordinate directions.
This connection will become much stronger when we introduce the gradient.
Partial Derivatives Do Not Give Every Direction
The pair
\[ f_x,\qquad f_y \]measures only the coordinate directions.
A surface can also be approached diagonally or along any other direction in the input plane.
Directional derivatives will generalize the coordinate-direction rates.
Common Error: Differentiating Every Variable
Consider
\[ f(x,y)=x^2y^3. \]For \(f_x\), \(y^3\) is held constant:
\[ \boxed{f_x=2xy^3}. \]It is incorrect to differentiate both \(x^2\) and \(y^3\) just because both appear in the expression.
Common Error: Dropping Constant Factors
If
\[ f(x,y)=yx^4, \]then with respect to \(x\),
\[ f_x=4yx^3. \]The factor \(y\) is constant with respect to \(x\), but it does not vanish. It stays as a constant multiplier.
Common Error: Keeping Terms That Should Vanish
For
\[ f(x,y)=x^3+5y^2, \]the \(x\)-partial is
\[ f_x=3x^2, \]because \(5y^2\) is constant with respect to \(x\).
Common Error: Misreading Mixed-Partial Order
In the notation
\[ f_{xy}, \]one common convention is: differentiate first with respect to \(x\), then differentiate the result with respect to \(y\).
The operator notation removes ambiguity:
\[ f_{xy} = \frac{\partial}{\partial y} \left( \frac{\partial f}{\partial x} \right). \]Common Error: Assuming Zero Partial Means No Change at All
If
\[ f_x(a,b)=0, \]the function has zero instantaneous rate in the \(x\)-direction at that point.
It may still change in the \(y\)-direction or in another direction.
One zero partial does not imply the function is locally constant.
Common Error: Ignoring the Domain
A derivative formula is meaningful only where the original function and the relevant derivative are defined.
For
\[ f(x,y)=\ln(x^2+y^2), \]the point \((0,0)\) is not in the domain, so partial derivatives there are not available.
A Reliable Procedure
- Identify the variable with respect to which you are differentiating.
- Treat all other independent variables as constants.
- Apply ordinary derivative rules to the active variable.
- Simplify the resulting expression.
- Repeat separately for any other requested partial derivatives.
- Check the domain of the original function and derivative.
- Evaluate at a point only after obtaining the derivative formula unless a direct limit is required.
Example: Full First-Partial Workflow
Let
\[ f(x,y)=x^3y^2+4x\sin y+e^{xy}. \]With respect to \(x\),
\[ f_x = 3x^2y^2+4\sin y+ye^{xy}. \]With respect to \(y\),
\[ f_y = 2x^3y+4x\cos y+xe^{xy}. \]Therefore,
\[ \boxed{ f_x=3x^2y^2+4\sin y+ye^{xy} } \]and
\[ \boxed{ f_y=2x^3y+4x\cos y+xe^{xy} }. \]Example: Full Second-Partial Workflow
Let
\[ f(x,y)=x^2y^3+3xy. \]First partials:
\[ f_x=2xy^3+3y, \] \[ f_y=3x^2y^2+3x. \]Differentiate again:
\[ f_{xx}=2y^3, \] \[ f_{xy}=6xy^2+3, \] \[ f_{yx}=6xy^2+3, \] \[ f_{yy}=6x^2y. \]Practice 1: Basic Polynomial
Find \(f_x\) and \(f_y\) for
\[ f(x,y)=x^3+4x^2y-5y^2. \]Practice 2: Product of Powers
Find \(f_x\) and \(f_y\) for
\[ f(x,y)=x^4y^5. \]Practice 3: Evaluate at a Point
For
\[ f(x,y)=x^2y+3y^2, \]find \(f_x(2,1)\) and \(f_y(2,1)\).
Practice 4: Exponential
Find the first partial derivatives of
\[ f(x,y)=e^{x+2y}. \]Practice 5: Trigonometric Function
Find \(f_x\) and \(f_y\) for
\[ f(x,y)=x\cos(xy). \]Practice 6: Rational Function
Find \(f_x\) and \(f_y\) for
\[ f(x,y)=\frac{x}{x+y}. \]Practice 7: Three Variables
For
\[ f(x,y,z)=x^2yz+xy^2z^3, \]find \(f_x\), \(f_y\), and \(f_z\).
Practice 8: Second Partials
For
\[ f(x,y)=x^2y^2+3x^3, \]find \(f_{xx}\), \(f_{xy}\), \(f_{yx}\), and \(f_{yy}\).
Practice 9: Interpretation
Suppose \(T(x,y)\) is temperature in degrees Celsius and \(x\) and \(y\) are measured in kilometers. Interpret
\[ T_x(4,2)=-3. \]Practice 10: Identify the Error
A student differentiates
\[ f(x,y)=x^2y^3 \]with respect to \(x\) and writes
\[ f_x=6xy^2. \]Explain the error and give the correct derivative.
Practice Answers
Practice 1
\[ \boxed{f_x=3x^2+8xy} \] \[ \boxed{f_y=4x^2-10y}. \]Practice 2
\[ \boxed{f_x=4x^3y^5} \] \[ \boxed{f_y=5x^4y^4}. \]Practice 3
First,
\[ f_x=2xy, \] \[ f_y=x^2+6y. \]Therefore,
\[ \boxed{f_x(2,1)=4} \]and
\[ \boxed{f_y(2,1)=10}. \]Practice 4
\[ \boxed{f_x=e^{x+2y}} \] \[ \boxed{f_y=2e^{x+2y}}. \]Practice 5
With respect to \(x\), use the product rule:
\[ \boxed{ f_x=\cos(xy)-xy\sin(xy) }. \]With respect to \(y\),
\[ \boxed{ f_y=-x^2\sin(xy) }. \]Practice 6
Using the quotient rule,
\[ \boxed{ f_x=\frac{y}{(x+y)^2} } \]and
\[ \boxed{ f_y=-\frac{x}{(x+y)^2} }. \]Practice 7
\[ \boxed{ f_x=2xyz+y^2z^3 } \] \[ \boxed{ f_y=x^2z+2xyz^3 } \] \[ \boxed{ f_z=x^2y+3xy^2z^2 }. \]Practice 8
First partials:
\[ f_x=2xy^2+9x^2, \] \[ f_y=2x^2y. \]Therefore,
\[ \boxed{f_{xx}=2y^2+18x}, \] \[ \boxed{f_{xy}=4xy}, \] \[ \boxed{f_{yx}=4xy}, \] \[ \boxed{f_{yy}=2x^2}. \]Practice 9
Near the point \((4,2)\), increasing \(x\) by one kilometer while holding \(y\) fixed decreases temperature at an instantaneous rate of approximately \(3\) degrees Celsius per kilometer.
Practice 10
When differentiating with respect to \(x\), the factor \(y^3\) must be treated as a constant. Therefore,
\[ \boxed{f_x=2xy^3}. \]The incorrect result differentiated the \(y\)-factor even though \(y\) was supposed to remain fixed.
What to Remember
Partial differentiation extends ordinary differentiation to functions with several independent variables.
- \(f_x\) measures local change in the \(x\)-direction while other inputs are fixed.
- \(f_y\) measures local change in the \(y\)-direction while other inputs are fixed.
- Ordinary derivative rules still apply to the active variable.
- Variables not currently being differentiated are treated as constants.
- First partials measure coordinate-direction sensitivity.
- Second partials measure how those rates themselves change.
- Mixed partials describe interaction between coordinate effects.
The essential computational rule is
\[ \boxed{ \text{differentiate one variable, hold the others fixed} }. \]Where We Go Next
Partial derivatives give rates of change along the coordinate axes, but multivariable functions can be approached in infinitely many directions.
The next lesson, Directional Derivatives, extends the idea of a partial derivative from the \(x\)- and \(y\)-directions to any chosen direction in the input space.