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Separable Equations
Use separation of variables to solve a differential equation.
Separation of Variables
We start with a definition and some examples.
The term ‘separable’ refers to the fact that the right-hand side of the equation can be separated into a function of \(x\) times a function of \(y.\) Examples of separable differential equations include
\[\begin{array}{l} \\ \\ y'=({x}^{2}-4)(3y+2) \\ y'=6{x}^{2}+4x \\ y'=\text{sec}\ y+\text{tan}\ y \\ y'=xy+3x-2y-6.\end{array}\]The second equation is separable with \(f(x)=6{x}^{2}+4x\) and \(g(y)=1,\) the third equation is separable with \(f(x)=1\) and \(g(y)=\text{sec}\ y+\text{tan}\ y,\) and the right-hand side of the fourth equation can be factored as \((x-2)(y+3),\) so it is separable as well. The third equation is also called an autonomous differential equation because the right-hand side of the equation is a function of \(y\) alone. If a differential equation is separable, then it is possible to solve the equation using the method of separation of variables.
Condensed — the full section is in OpenStax Calculus Volume 2.
Applications of Separation of Variables
Many interesting problems can be described by separable equations. We illustrate two types of problems: solution concentrations and Newton’s law of cooling.
Condensed — the full section is in OpenStax Calculus Volume 2.
Key Concepts
- A separable differential equation is any equation that can be written in the form \(y'=f(x)g(y).\)
- The method of separation of variables is used to find the general solution to a separable differential equation.
Key Equations
| Separable differential equation | \({y}^{'}=f(x)g(y)\) |
| Solution concentration | \(\frac{du}{dt}=\text{INFLOW RATE}-\text{OUTFLOW RATE}\) |
| Newton’s law of cooling | \(\frac{dT}{dt}=k(T-{T}_{s})\) |
Separable Equations
Solve the following initial-value problems with the initial condition \({y}_{0}=0\) and graph the solution.
Find the general solution to the differential equation.
Find the solution to the initial-value problem.
For the following problems, use a software program or your calculator to generate the directional fields. Solve explicitly and draw solution curves for several initial conditions. Are there some critical initial conditions that change the behavior of the solution?
For the following problems, use Newton’s law of cooling.
For Exercises 159—162, assume a cooling constant of \(k=-0.125\) and assume time \(t\) is in minutes.
Practice (40)
Try each one on paper first. Reveal the answer to check; verified ones can be opened in the solver for every step.
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Find a general solution to the differential equation \(y'=({x}^{2}-4)(3y+2)\) using the method of separation of variables.
Fi àwọn àgbèwọlé hàn
Follow the five-step method of separation of variables.
- In this example, \(f(x)={x}^{2}-4\) and \(g(y)=3y+2.\) Setting \(g(y)=0\) gives \(y=-\frac{2}{3}\) as a constant solution.
- Rewrite the differential equation in the form
\[\frac{dy}{3y+2}=({x}^{2}-4)dx.\] - Integrate both sides of the equation:
\[\int \frac{dy}{3y+2}=\int ({x}^{2}-4)\ dx.\]
Let \(u=3y+2.\) Then \(du=3\frac{dy}{dx}dx,\) so the equation becomes
\[\begin{array}{lll}\frac{1}{3}\int \frac{1}{u}du & = & \frac{1}{3}{x}^{3}-4x+C \\ \frac{1}{3}\ \text{ln}|u| & = & \frac{1}{3}{x}^{3}-4x+C \\ \frac{1}{3}\ \text{ln}|3y+2| & = & \frac{1}{3}{x}^{3}-4x+C.\end{array}\] - To solve this equation for \(y,\) first multiply both sides of the equation by \(3.\)
\[\text{ln}|3y+2|={x}^{3}-12x+3C\]
Now we use some logic in dealing with the constant \(C.\) Since \(C\) represents an arbitrary constant, \(3C\) also represents an arbitrary constant. If we call the second arbitrary constant \({C}_{1},\) the equation becomes
\[\text{ln}|3y+2|={x}^{3}-12x+{C}_{1}.\]
Now exponentiate both sides of the equation (i.e., make each side of the equation the exponent for the base \(e).\)
\[\begin{array}{lll}{e}^{\text{ln}|3y+2|} & = & {e}^{{x}^{3}-12x+{C}_{1}} \\ |3y+2| & = & {e}^{{C}_{1}}{e}^{{x}^{3}-12x}\end{array}\]
Again define a new constant \({C}_{2}={e}^{{c}_{1}}\) (note that \({C}_{2}>0)\text{:}\)
\[|3y+2|={C}_{2}{e}^{{x}^{3}-12x}.\]
This corresponds to two separate equations: \(3y+2={C}_{2}{e}^{{x}^{3}-12x}\) and \(3y+2=\text{-}{C}_{2}{e}^{{x}^{3}-12x}.\)
The solution to either equation can be written in the form \(y=\frac{-2\pm {C}_{2}{e}^{{x}^{3}-12x}}{3}.\)
Since \({C}_{2}>0,\) it does not matter whether we use plus or minus, so the constant can actually have either sign. Furthermore, the subscript on the constant \(C\) is entirely arbitrary, and can be dropped. Therefore the solution can be written as
\[y=\frac{-2+C{e}^{{x}^{3}-12x}}{3}.\] - No initial condition is imposed, so we are finished.
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Use the method of separation of variables to find a general solution to the differential equation \(y'=2xy+3y-4x-6.\)
Fi àwọn àgbèwọlé hàn
\(y=2+C{e}^{{x}^{2}+3x}\)
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Using the method of separation of variables, solve the initial-value problem
\[y'=(2x+3)({y}^{2}-4),\ y(0)=-1.\]Fi àwọn àgbèwọlé hàn
Follow the five-step method of separation of variables.
- In this example, \(f(x)=2x+3\) and \(g(y)={y}^{2}-4.\) Setting \(g(y)=0\) gives \(y=\pm 2\) as constant solutions.
- Divide both sides of the equation by \({y}^{2}-4\) and multiply by \(dx.\) This gives the equation
\[\frac{dy}{{y}^{2}-4}=(2x+3)\ dx.\] - Next integrate both sides:
\[\int \frac{1}{{y}^{2}-4}\ dy=\int (2x+3)\ dx.\]
To evaluate the left-hand side, use the method of partial fraction decomposition. This leads to the identity
\[\frac{1}{{y}^{2}-4}=\frac{1}{4}(\frac{1}{y-2}-\frac{1}{y+2}).\]
Then becomes
\[\begin{array}{lll}\frac{1}{4}\int (\frac{1}{y-2}-\frac{1}{y+2})\ dy & = & \int (2x+3)\ dx \\ \frac{1}{4}(\text{ln}|y-2|-\text{ln}|y+2|) & = & {x}^{2}+3x+C.\end{array}\]
Multiplying both sides of this equation by \(4\) and replacing \(4C\) with \({C}_{1}\) gives
\[\begin{array}{lll}\text{ln}|y-2|-\text{ln}|y+2| & = & 4{x}^{2}+12x+{C}_{1} \\ \text{ln}|\frac{y-2}{y+2}| & = & 4{x}^{2}+12x+{C}_{1}.\end{array}\] - It is possible to solve this equation for y. First exponentiate both sides of the equation and define \({C}_{2}={e}^{{C}_{1}}\text{:}\)
\[|\frac{y-2}{y+2}|={C}_{2}{e}^{4{x}^{2}+12x}.\]
Next we can remove the absolute value and let \({C}_{2}\) be either positive or negative. Then multiply both sides by \(y+2.\)
\[\begin{array}{l} \\ \\ y-2={C}_{2}(y+2){e}^{4{x}^{2}+12x} \\ y-2={C}_{2}y{e}^{{}^{4{x}^{2}+12x}}+2{C}_{2}{e}^{{}^{4{x}^{2}+12x}}.\end{array}\]
Now collect all terms involving y on one side of the equation, and solve for \(y\text{:}\)
\[\begin{array}{lll}y-{C}_{2}y{e}^{4{x}^{2}+12x} & = & 2+2{C}_{2}{e}^{4{x}^{2}+12x} \\ y(1-{C}_{2}{e}^{4{x}^{2}+12x}) & = & 2+2{C}_{2}{e}^{4{x}^{2}+12x} \\ y & = & \frac{2+2{C}_{2}{e}^{4{x}^{2}+12x}}{1-{C}_{2}{e}^{4{x}^{2}+12x}}.\end{array}\] - To determine the value of \({C}_{2},\) substitute \(x=0\) and \(y=-1\) into the general solution. Alternatively, we can put the same values into an earlier equation, namely the equation \(\frac{y-2}{y+2}={C}_{2}{e}^{4{x}^{2}+12}.\) This is much easier to solve for \({C}_{2}\text{:}\)
\[\begin{array}{lll}\frac{y-2}{y+2} & = & {C}_{2}{e}^{4{x}^{2}+12x} \\ \frac{-1-2}{-1+2} & = & {C}_{2}{e}^{4{(0)}^{2}+12(0)} \\ {C}_{2} & = & -3.\end{array}\]
Therefore the solution to the initial-value problem is
\[y=\frac{2-6{e}^{4{x}^{2}+12x}}{1+3{e}^{4{x}^{2}+12x}}.\]
A graph of this solution appears in .
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Find the solution to the initial-value problem
\[6y'=(2x+1)({y}^{2}-2y-8),\ y(0)=-3\]using the method of separation of variables.
Fi àwọn àgbèwọlé hàn
\(y=\frac{4+14{e}^{{x}^{2}+x}}{1-7{e}^{{x}^{2}+x}}\)
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A tank containing \(100\ \text{L}\) of a brine solution initially has \(4\ \text{kg}\) of salt dissolved in the solution. At time \(t=0,\) another brine solution flows into the tank at a rate of \(2\ \text{L/min}\text{.}\) This brine solution contains a concentration of \(0.5\ \text{kg/L}\) of salt. At the same time, a stopcock is opened at the bottom of the tank, allowing the combined solution to flow out at a rate of \(2\ \text{L/min},\) so that the level of liquid in the tank remains constant (). Find the amount of salt in the tank as a function of time (measured in minutes), and find the limiting amount of salt in the tank, assuming that the solution in the tank is well mixed at all times.
Fi àwọn àgbèwọlé hàn
First we define a function \(u(t)\) that represents the amount of salt in kilograms in the tank as a function of time. Then \(\frac{du}{dt}\) represents the rate at which the amount of salt in the tank changes as a function of time. Also, \(u(0)\) represents the amount of salt in the tank at time \(t=0,\) which is \(4\) kilograms.
The general setup for the differential equation we will solve is of the form
\[\frac{du}{dt}=\text{INFLOW RATE}-\text{OUTFLOW RATE}.\]INFLOW RATE represents the rate at which salt enters the tank, and OUTFLOW RATE represents the rate at which salt leaves the tank. Because solution enters the tank at a rate of \(2\) L/min, and each liter of solution contains \(0.5\) kilogram of salt, every minute \(2(0.5)=1\ \text{kilogram}\) of salt enters the tank. Therefore INFLOW RATE = \(1.\)
To calculate the rate at which salt leaves the tank, we need the concentration of salt in the tank at any point in time. Since the actual amount of salt varies over time, so does the concentration of salt. However, the volume of the solution remains fixed at 100 liters. The number of kilograms of salt in the tank at time \(t\) is equal to \(u(t).\) Thus, the concentration of salt is \(\frac{u(t)}{100}\) kg/L, and the solution leaves the tank at a rate of \(2\) L/min. Therefore salt leaves the tank at a rate of \(\frac{u(t)}{100}\cdot 2=\frac{u(t)}{50}\) kg/min, and OUTFLOW RATE is equal to \(\frac{u(t)}{50}.\) Therefore the differential equation becomes \(\frac{du}{dt}=1-\frac{u}{50},\) and the initial condition is \(u(0)=4.\) The initial-value problem to be solved is
\[\frac{du}{dt}=1-\frac{u}{50},\ u(0)=4.\]The differential equation is a separable equation, so we can apply the five-step strategy for solution.
Step 1. Setting \(1-\frac{u}{50}=0\) gives \(u=50\) as a constant solution. Since the initial amount of salt in the tank is \(4\) kilograms, this solution does not apply.
Step 2. Rewrite the equation as
\[\frac{du}{dt}=\frac{50-u}{50}.\]Then multiply both sides by \(dt\) and divide both sides by \(50-u\text{:}\)
\[\frac{du}{50-u}=\frac{dt}{50}.\]Step 3. Integrate both sides:
\[\begin{array}{lll}\int \frac{du}{50-u} & = & \int \frac{dt}{50} \\ -\text{ln}|50-u| & = & \frac{t}{50}+C.\end{array}\]Step 4. Solve for \(u(t)\text{:}\)
\[\begin{array}{lll}\text{ln}|50-u| & = & -\frac{t}{50}-C \\ {e}^{\text{ln}|50-u|} & = & {e}^{\text{-}(t\text{/}50)-C} \\ |50-u| & = & {C}_{1}{e}^{\text{-}t\text{/}50}.\end{array}\]Eliminate the absolute value by allowing the constant to be either positive or negative:
\[50-u={C}_{1}{e}^{\text{-}t\text{/}50}.\]Finally, solve for \(u(t)\text{:}\)
\[u(t)=50-{C}_{1}{e}^{\text{-}t\text{/}50}.\]Step 5. Solve for \({C}_{1}\text{:}\)
\[\begin{array}{lll}u(0) & = & 50-{C}_{1}{e}^{-0\text{/}50} \\ 4 & = & 50-{C}_{1} \\ {C}_{1} & = & 46.\end{array}\]The solution to the initial value problem is \(u(t)=50-46{e}^{\text{-}t\text{/}50}.\) To find the limiting amount of salt in the tank, take the limit as \(t\) approaches infinity:
\[\begin{array}{ll}\underset{t\to \infty }{\text{lim}}u(t) & =50-46{e}^{\text{-}t\text{/}50} \\ & =50-46(0) \\ & =50.\end{array}\]Note that this was the constant solution to the differential equation. If the initial amount of salt in the tank is \(50\) kilograms, then it remains constant. If it starts at less than 50 kilograms, then it approaches 50 kilograms over time.
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A tank contains \(3\) kilograms of salt dissolved in \(75\) liters of water. A salt solution of \(0.4\ \text{kg salt/L}\) is pumped into the tank at a rate of \(6\ \text{L/min}\) and is drained at the same rate. Solve for the salt concentration at time \(t.\) Assume the tank is well mixed at all times.
Fi àwọn àgbèwọlé hàn
Initial value problem:
\(\frac{du}{dt}=2.4-\frac{2u}{25},\ u(0)=3\)
\(\text{Solution:}\ u(t)=30-27{e}^{\text{-}2t\text{/}25}\)
\(\text{Concentration: }30-27{e}^{\frac{-2t}{25}}\) -
A pizza is removed from the oven after baking thoroughly, and the temperature of the pizza when it comes out of the oven is \(200\text{^{\circ}}\text{F}\text{.}\) The temperature of the kitchen is \(75\text{^{\circ}}\text{F},\) and after \(1\) minute the temperature of the pizza is \(190\text{^{\circ}}\text{F}\text{.}\) We would like to wait until the temperature of the pizza reaches \(150\text{^{\circ}}\text{F}\) before cutting and serving it (). How much longer will we have to wait?
Fi àwọn àgbèwọlé hàn
The ambient temperature (surrounding temperature) is \(75\text{^{\circ}}\text{F},\) so \({T}_{s}=75.\) The temperature of the pizza when it comes out of the oven is \(200\text{^{\circ}}\text{F},\) which is the initial temperature (i.e., initial value), so \({T}_{0}=200.\) Therefore becomes
\[\frac{dT}{dt}=k(T-75),\ T(0)=200.\]To solve the differential equation, we use the five-step technique for solving separable equations.
- Setting the right-hand side equal to zero gives \(T=75\) as a constant solution. Since the pizza starts at \(200\text{^{\circ}}\text{F},\) this is not the solution we are seeking.
- Rewrite the differential equation by multiplying both sides by \(dt\) and dividing both sides by \(T-75\text{:}\)
\[\frac{dT}{T-75}=kdt.\] - Integrate both sides:
\[\begin{array}{lll}\int \frac{dT}{T-75} & = & \int kdt \\ \text{ln}|T-75| & = & kt+C.\end{array}\] - Solve for \(T\) by first exponentiating both sides:
\[\begin{array}{lll}{e}^{\text{ln}|T-75|} & = & {e}^{kt+C} \\ |T-75| & = & {C}_{1}{e}^{kt} \\ T-75 & = & {C}_{1}{e}^{kt} \\ T(t) & = & 75+{C}_{1}{e}^{kt}.\end{array}\] - Solve for \({C}_{1}\) by using the initial condition \(T(0)=200\text{:}\)
\[\begin{array}{lll}T(t) & = & 75+{C}_{1}{e}^{kt} \\ T(0) & = & 75+{C}_{1}{e}^{k(0)} \\ 200 & = & 75+{C}_{1} \\ {C}_{1} & = & 125.\end{array}\]
Therefore the solution to the initial-value problem is
\[T(t)=75+125{e}^{kt}.\]
To determine the value of \(k,\) we need to use the fact that after \(1\) minute the temperature of the pizza is \(190\text{^{\circ}}\text{F}\text{.}\) Therefore \(T(1)=190.\) Substituting this information into the solution to the initial-value problem, we have
\[\begin{array}{lll}T(t) & = & 75+125{e}^{kt} \\ T(1) & = & 190=75+125{e}^{k} \\ 115 & = & 125{e}^{k} \\ \frac{115}{125} & = & \frac{23}{25}={e}^{k} \\ \text{ln}\ {e}^{k} & = & \text{ln}\ (\frac{23}{25}) \\ k & = & \ \text{ln}\ (\frac{23}{25})\approx -.08338\end{array}\]
So now we have \(T(t)=75+125{e}^{-.08338t}.\) When is the temperature \(150\text{^{\circ}}\text{F?}\) Solving for \(t,\) we find
\[\begin{array}{lll}T(t) & = & 75+125{e}^{-.08338t} \\ 150 & = & 75+125{e}^{-.08338t} \\ 75 & = & 125{e}^{-.08338t} \\ \frac{75}{125} & = & \frac{3}{5}={e}^{-.08338t} \\ -.08338t & = & \text{ln}\ \frac{3}{5} \\ t & = & \frac{\text{ln}\left(\frac{3}{5}\right)}{-.08338}\approx 6.12.\end{array}\]
Therefore we need to wait an additional \(6.12\) minutes (after the temperature of the pizza reached \(200\text{^{\circ}}\text{F}).\) That should be just enough time to finish this calculation.
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A cake is removed from the oven after baking thoroughly, and the temperature of the cake when it comes out of the oven is \(450\text{^{\circ}}\text{F}\text{.}\) The temperature of the kitchen is \(70\text{^{\circ}}\text{F},\) and after \(10\) minutes the temperature of the cake is \(330\text{^{\circ}}\text{F}\text{.}\)
- Write the appropriate initial-value problem to describe this situation.
- Solve the initial-value problem for \(T(t).\)
- How long will it take until the temperature of the cake is within \(5\text{^{\circ}}\text{F}\) of room temperature?
Fi àwọn àgbèwọlé hàn
- Initial value problem
\(\frac{dT}{dt}=k(T-70),\ T(0)=450\) - \(T(t)=70+380{e}^{kt}\)
- Approximately \(114\) minutes.
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\(\frac{dy}{dt}=y+1\)
Fi àwọn àgbèwọlé hàn
\(y={e}^{t}-1\)
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\(\frac{dy}{dt}=y-1\)
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\(\frac{dy}{dt}=-y+1\)
Fi àwọn àgbèwọlé hàn
\(y=1+C{e}^{\text{-}t}\)
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\(\frac{dy}{dt}=\text{-}y-1\)
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\({x}^{2}y'=(x+1)y\)
Fi àwọn àgbèwọlé hàn
\(y=Cx{e}^{-1\text{/}x}\)
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\(y'=\text{tan}(y)x\)
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\(y'=2x{y}^{2}\)
Fi àwọn àgbèwọlé hàn
\(y=\frac{1}{C-{x}^{2}}\)
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\(\frac{dy}{dt}=y\ \text{cos}(3t+2)\)
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\(2x\frac{dy}{dx}={y}^{2}\)
Fi àwọn àgbèwọlé hàn
\(y=-\frac{2}{C+\text{ln}\ x}\)
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\(y'={e}^{y}{x}^{2}\)
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\((1+x)y'=(x+2)(y-1)\)
Fi àwọn àgbèwọlé hàn
\(y=C{e}^{x}(x+1)+1\)
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\(\frac{dx}{dt}=3{t}^{2}({x}^{2}+4)\)
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\(t\frac{dy}{dt}=\sqrt{1-{y}^{2}}\)
Fi àwọn àgbèwọlé hàn
\(y=\text{sin}(\text{ln}\ t+C)\)
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\(y'={e}^{x}{e}^{y}\)
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\(y'={e}^{y-x},y(0)=0\)
Fi àwọn àgbèwọlé hàn
\(y=\text{-}\text{ln}({e}^{\text{-}x})\)
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\(y'={y}^{2}(x+1),y(0)=2\)
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\(\frac{dy}{dx}={y}^{3}x{e}^{{x}^{2}},y(0)=1\)
Fi àwọn àgbèwọlé hàn
\(y=\frac{1}{\sqrt{2-{e}^{{x}^{2}}}}\)
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\(\frac{dy}{dt}={y}^{2}{e}^{x}\text{sin}(3x),y(0)=1\)
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\(y'=\frac{x}{{\text{sech}}^{2}y},y(0)=0\)
Fi àwọn àgbèwọlé hàn
\(y={\text{tanh}}^{-1}(\frac{{x}^{2}}{2})\)
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\(y'=2xy(1+2y),y(0)=-1\)
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\(\frac{dx}{dt}=\text{ln}(t)\sqrt{1-{x}^{2}},x(1)=0\)
Fi àwọn àgbèwọlé hàn
\(x=\text{sin}(1-t+t\ \text{ln}\ t)\)
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\(y'=3{x}^{2}({y}^{2}+4),y(0)=0\)
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\(y'={e}^{y}{5}^{x},y(0)=\text{ln}(\text{ln}(5))\)
Fi àwọn àgbèwọlé hàn
\(y=\text{ln}(\text{ln}(5))-\text{ln}(2-{5}^{x})\)
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\(y'=-2x\ \text{tan}(y),y(0)=\frac{\pi }{6}\)
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[T] \(y'=1-2y\)
Fi àwọn àgbèwọlé hàn
\(y=C{e}^{-2x}+\frac{1}{2}\)
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[T] \(y'={y}^{2}{x}^{3}\)
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[T] \(y'={y}^{3}{e}^{x}\)
Fi àwọn àgbèwọlé hàn
\(y=\frac{1}{\sqrt{2}\sqrt{C-{e}^{x}}}\)
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[T] \(y'={e}^{y}\)
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[T] \(y'=y\ \text{ln}(x)\)
Fi àwọn àgbèwọlé hàn
\(y=C{e}^{\text{-}x}{x}^{x}\)
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Most drugs in the bloodstream decay according to the equation \(y'=cy,\) where \(y\) is the concentration of the drug in the bloodstream. If the half-life of a drug is \(2\) hours, what fraction of the initial dose remains after \(6\) hours?
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A drug is administered intravenously to a patient at a rate \(r\) mg/h and is cleared from the body at a rate proportional to the amount of drug still present in the body, \(d\). Set up and solve the differential equation, assuming there is no drug initially present in the body.
Fi àwọn àgbèwọlé hàn
\(y=\frac{r}{d}(1-{e}^{\text{-}dt})\)
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[T] How often should a drug be taken if its dose is \(3\) mg, it is cleared at a rate \(c=0.1\) mg/h, and \(1\) mg is required to be in the bloodstream at all times?
Symbols used here
Instantaneous rate of change; slope of the graph.
Prime notation for derivatives with respect to x (or t).
1/360 of a full turn. 180° = π radians.
Ratio of a circle's circumference to its diameter, 3.14159…
2.71828…, the base whose exponential is its own derivative.
Not a number: "grows without bound" in limits and intervals.
Ratios of sides in a right triangle; coordinates on the unit circle.
The exponent b must be raised to for x; ln uses base e.
Add a_k for k = 1 up to n.
The value f(x) approaches as x approaches a.
Antiderivative (indefinite) or signed area from a to b (definite).
Constants of integration fixed by initial conditions.
How to: Separable Equations
- Use separation of variables to solve a differential equation.
- Solve applications using separation of variables.
- Check for any values of
- Rewrite the differential equation in the form
- Integrate both sides of the equation.
- Solve the resulting equation for
- If an initial condition exists, substitute the appropriate values for
- In this example,
Questions people ask
What is a derivative in one sentence?
The slope of the graph at a point — the rate at which the output is changing there. Speed is the derivative of position.
What is an integral in one sentence?
The accumulated total of a rate — the area under the curve. Distance travelled is the integral of speed.
Why are derivatives and integrals opposites?
That is the fundamental theorem of calculus: accumulating a rate and then measuring how fast the accumulation grows gets you back the rate. Integration undoes differentiation up to a constant.
When do I use substitution and when integration by parts?
Substitution when part of the integrand is the derivative of another part (u and du both present). Parts when the integrand is a product of two unrelated kinds of function — a polynomial times an exponential, log or trig function.
Wárá
Parts of this page are adapted from OpenStax Calculus Volume 2 (CC BY-NC-SA 4.0). Condensed and re-explained here; errors are ours.
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