Coordinate bounds of the solid
The region is defined by three independent intervals: , , and . Together these describe a rectangular box aligned with the coordinate axes.
Khan Academy · YouTube · 10:38
This 120-second clip introduces a rectangular solid with bounds , , and . The instructor writes the bounds, sketches the corresponding box in xyz-space, and notes that although basic geometry already gives the volume, the example is being used to prepare viewers for triple integrals and their relation to double integrals. The volume is computed geometrically as 24 cubic units. No actual triple-integral notation is written within this clip. This 120-second whiteboard clip introduces the meaning of a triple integral through a rectangular box bounded by , , and . A small cube inside the box is used as the basic volume element, with side lengths , , and . The speaker defines the volume differential , notes that the factors can be reordered because multiplication is commutative, and then begins the integration process conceptually by summing first in the -direction to form a column. The clip stops before any explicit iterated integral notation is written. This 120-second whiteboard segment introduces a triple integral as a way to compute the volume of a rectangular box. The board shows the bounds , , and the volume element dV = dx dy dz. The instructor builds the iterated integral from the inside out: first integrate in z from 0 to 2 to get the height of a column, then integrate in y from 0 to 4 to form a sheet parallel to the zy-plane, and finally integrate in x from 0 to 3 to obtain the whole solid. The final setup is . The clip ends before the numerical evaluation is carried out. This 120-second whiteboard clip computes the volume of a rectangular box with bounds , , using the iterated triple integral \, dz \, dy \, dx. The speaker first explains that the missing integrand is 1, then integrates from the inside out: z gives 2, y gives 8, and x gives 24. Midway through, the clip explicitly connects the result after the z-step to a double integral with constant height , emphasizing that for this example the triple integral reduces to the same kind of volume-under-a-surface computation seen earlier. This 120-second whiteboard clip shifts from a completed triple-integral volume calculation for a rectangular box to the setup for mass with variable density. The board shows the box , , and the evaluated integral . The speaker then introduces a non-uniform density , explains that a small mass equals local density times a small volume element, writes , and notes that in Cartesian coordinates is width times height times depth, though its form changes in other coordinate systems. This video segment introduces the concept of calculating mass using a density function and differential volume elements in rectangular coordinates. The formula for differential mass is presented, along with a visual representation of the region and volume element.
Use the learning inspector for key ideas and moments, or open the reading tabs for the complete notes.
Generated from the video's visuals and explanation; not verbatim speech.
The clip opens with a spoken setup: the goal is to find the volume of a solid whose coordinate ranges are about to be specified.
Three inequalities are written in green: , , and . These define an axis-aligned rectangular box in three-dimensional space.
The instructor points out that elementary geometry would already solve the problem by multiplying the three side lengths, but the real purpose is pedagogical: to acclimate the viewer to the form of a triple integral and its connection to a double integral.
A three-axis coordinate frame is drawn and labeled , , and , establishing the spatial setting for the region.
Using the stated bounds, the sketch adds tick marks and dashed edges to form the rectangular solid. The lower face lies in the plane , and the opposite face lies at ; the horizontal extents are in the -direction and in the -direction.
The volume is then computed directly from the geometry: the base area is , and multiplying by the height gives cubic units.
The clip ends just as the instructor begins to move beyond the purely geometric computation toward the integral viewpoint.
The clip opens by asking what a triple integral means. On screen, a dashed rectangular box sits in a 3D coordinate system, with the bounds , , and written at top left.
To answer the question, the speaker isolates one tiny cube inside the larger box. This small cube is the local volume piece whose size will be measured in the three coordinate directions.
The side lengths are assigned one by one: width , height , and depth . The speaker briefly misspeaks by calling the height , then corrects it because the drawn -axis is the vertical direction.
With those three edge lengths identified, the infinitesimal volume is named and written as . The speaker also remarks that the factors may be reordered because ordinary multiplication is associative and order does not matter.
The explanation then broadens from one cube to the integral idea: an integral is described as an infinite sum of infinitely small pieces such as , , and .
Finally, the first summation direction is chosen. The speaker says to add the small cubes along the -axis, building a column-like intermediate volume before any further integration steps are taken.
The clip opens on a digital blackboard showing a rectangular box in 3D space. At the top left, the green inequalities , , and define the region. At the top right, the cyan formula names the infinitesimal volume element. A small cube drawn inside the larger dashed box visually represents one such element.
The instructor begins constructing the integral from the inside outward. He asks for the lowest and highest -values in the box and identifies them as and . This motivates the innermost integral , which corresponds to stacking tiny cubes vertically through the height of the box.
He then fixes the order of integration by writing the differentials as , then , then . The spoken explanation makes clear that this ordering is intentional: is integrated first, second, and last. Thus the emerging expression is an iterated integral whose nesting mirrors successive geometric summations.
With only the inner -integral in place, the instructor interprets its meaning. For any fixed and , gives the volume of one vertical column. Because the -bounds are constant, this column volume simplifies to : height times base area . This is a key conceptual step from infinitesimal cube to finite-height column.
Next, he adds the middle integral in the -direction. Since the box satisfies , the new layer is . Geometrically, this sums many adjacent columns side by side in the -direction, producing a sheet parallel to the -plane. The written expression becomes .
Finally, the outer integral is added in the -direction using the bound . This stacks the previously formed sheets along until the entire rectangular solid is recovered. The completed setup on the board is , which the speaker identifies as the volume of the whole figure.
The segment ends just as the instructor says that evaluating the integral is straightforward. No numerical evaluation is shown within this clip, so the mathematical content here is the construction and interpretation of the triple integral rather than its final computed value.
The clip opens on a black digital whiteboard with a dashed rectangular box drawn in a 3D coordinate system. At the upper left, the bounds are written in green: , , and . At the upper center, the volume element is written as . To the right, the iterated integral is shown as .
The speaker points out that no function is written inside the integral, then explains that this means the integrand is implicitly . A red is added before , making the integral .
The first integration is with respect to . Since the antiderivative of with respect to is , the board shows . Evaluating at the limits gives , so the triple integral reduces to .
The speaker then emphasizes the conceptual link to earlier material: after the -step, what remains is a double integral. On the right side, the function is written, identifying the top of the box as a constant-height surface above the rectangle in the -plane.
This connection is explained verbally: is a function of and , but here it is constant and independent of both. Thus the volume under the surface over the base region is exactly the same computation that the reduced double integral represents.
The evaluation continues with the -integral. The antiderivative of with respect to is , giving . The remaining single integral is therefore .
Finally, the antiderivative of with respect to is , so . The speaker states the result as units cubed, which is the volume of the rectangular box.
The clip ends by raising the next question—why use triple integrals at all—without answering it within this segment.
The clip opens on a worked volume example for a rectangular solid. On the left is a 3D box with bounds , , and ; on the right is the iterated integral and its evaluation to . The speaker points out that when the integrand is constant inside the volume, a lower-dimensional integral could have sufficed for volume, but the lesson is now changing goals: instead of volume, we want mass.
The next distinction is between uniform and non-uniform density. If density were constant everywhere, total mass would simply be that constant density multiplied by the total volume. But the speaker says to imagine a substance whose density changes from point to point, such as a gas or a mixed material. That motivates treating density as a function of position rather than as a single number.
The board then introduces the standard physics symbol for density and writes a concrete example: . This means the density at a point depends on all three coordinates. The earlier box remains the region of interest, so the same rectangular solid is now being reused, not to integrate the constant function , but to prepare for integrating a variable density over the solid.
From that density function, the speaker derives the local mass element. He argues by units and by interpretation: density has units like mass per volume, so multiplying density at a point by a tiny volume gives a tiny amount of mass. He writes this as , or more conceptually . This is the basic building block for a triple-integral mass calculation.
Finally, the clip explains what means in the current Cartesian setting. The speaker identifies it with width times height times depth, corresponding to the small side lengths of a tiny rectangular piece inside the box. He also warns that is not always written as ; in other coordinate systems its expression changes. The segment therefore ends after setting up the mass integrand, without yet carrying out the full triple integral for mass.
To find the mass in rectangular coordinates, multiply the density function by the differential volume element .
The diagram shows a 3D box with dimensions , , , and a small cube representing the differential volume element .
The region is defined by three independent intervals: , , and . Together these describe a rectangular box aligned with the coordinate axes.
Although the volume can be found immediately by geometry, the instructor chooses this simple solid to help viewers become familiar with what a triple integral looks like and how it relates to a double integral before tackling more complicated regions.
For a rectangular solid, volume equals the product of its three side lengths. Here the side lengths are 3, 4, and 2, so the volume is cubic units.
The spoken introduction refers to a cube, but the displayed bounds give unequal side lengths 3, 4, and 2. Mathematically, the object shown is a rectangular box, not a cube.
The video introduces a triple integral by asking what it means geometrically. The answer given here is that it is built from summing tiny volume pieces inside a three-dimensional region, beginning with one small rectangular cube inside a larger box.
The example region is a Cartesian rectangular box with bounds , , and . This simple shape is used before moving to more complicated variable boundaries.
A tiny cube is drawn somewhere inside the larger box. Its role is to represent one infinitesimal chunk of volume that will later be summed repeatedly to recover the whole region.
The cube's width is , its height is , and its depth is . The correction matters because the vertical axis in the drawing is , so height must correspond to , not .
The infinitesimal volume of the small cube is called the volume differential and is written as the product of its three side lengths.
Since is presented as a product, the speaker notes that , , and can be switched in order without changing the product. This is a statement about multiplication of the differential factors.
The clip explains integrals conceptually as tools for taking infinite sums of infinitely small quantities such as , , and . This is the bridge from one tiny cube to the full triple-integral idea.
The speaker chooses to begin by adding the small cubes in the -direction, producing the volume of a column. The clip stops before writing the corresponding iterated integral notation.
The video defines the infinitesimal volume of a small rectangular cube inside a 3D box by . The accompanying drawing of a tiny cube inside the larger dashed box shows that triple integration is built by summing many such small volume pieces.
The solid being integrated over is the axis-aligned rectangular box given by , , and . These constant inequalities supply the limits used later in the iterated integral.
The instructor deliberately writes first, then , then , explaining that this means the integral is taken with respect to first, then , then . The order is tied to a geometric buildup from vertical columns to sheets to the full solid.
For fixed and , the inner integral computes the volume of one vertical column. Since the height is constantly 2, the column volume is . This step turns the abstract integral into a concrete geometric piece of the box.
After obtaining column volumes, the next integral sums them in the -direction from 0 to 4. The speaker describes the result as the volume of a sheet parallel to the -plane, showing how one-dimensional summation builds a two-dimensional slab inside the box.
The last integral adds those sheets in the -direction from 0 to 3. This completes the transition from a single infinitesimal cube to a column, then a sheet, then the entire rectangular solid, yielding the full volume integral.
Putting the three stages together, the video arrives at the iterated triple integral . This expression is presented as the volume of the whole box, although the clip ends before evaluating it numerically.
The example computes the volume of the box with bounds , , and . Because volume is being measured, the integrand is the constant , and the volume element is written as . The displayed iterated integral is .
The speaker explicitly notes that nothing is written under the integral sign, but that this is equivalent to inserting a factor of . In other words, is treated as . This is the standard setup when an integral is being used to compute volume.
The method shown is to integrate from the innermost differential outward. First, . Then the problem becomes . Next, , leaving .
After the -integration, the remaining expression is . The speaker identifies this as the same type of double integral used previously to compute volume under a surface. For this box, the surface height is constant.
The board writes to describe the top face of the box. The speaker explains that this is a constant function, independent of and . Therefore the volume under the surface over the rectangular base is computed by integrating the constant height across the -region.
Explore conditions, steps and evidence. Supplementary explanations are labeled separately from content shown in the video.
Green handwritten inequality `` is written in the upper-left area.
The speaker says that x is greater than or equal to 0 and less than or equal to 3.
x
Coordinate variable for one side length of the rectangular solid; its interval is from 0 to 3.
Green handwritten inequality `` is written below the x-bound.
The speaker says that y is greater than or equal to 0 and less than or equal to 4.
y
Coordinate variable for a second side length of the rectangular solid; its interval is from 0 to 4.
Green handwritten inequality `` is written below the y-bound.
The speaker says that z is greater than or equal to 0 and less than or equal to 2.
z
Coordinate variable for the height of the rectangular solid; its interval is from 0 to 2.
Three green axes are drawn and labeled x, y, and z in a three-dimensional coordinate sketch.
The speaker identifies the drawn axes as the x-axis, z-axis, and y.
x,y,z
Labels of the three mutually perpendicular coordinate axes used to draw the rectangular solid.
Three-dimensional Cartesian coordinate system
Top-left handwritten inequalities include .
The speaker later labels one edge of the small cube as .
x
Cartesian coordinate along the depth direction of the large rectangular box in this clip.
Top-left handwritten inequalities include .
The speaker labels one edge of the small cube as .
y
Cartesian coordinate along the width direction of the large rectangular box in this clip.
Top-left handwritten inequalities include .
The speaker says the height is and that is up and down.
z
Cartesian vertical coordinate, used for the height direction of the large rectangular box.
The speaker says, "And then its depth is dx."
The final written formula is , containing .
dx
Infinitesimal length increment in the -direction, corresponding to the depth of the small cube.
The speaker says, "Let's say that its width is dy."
The final written formula is , containing .
dy
Infinitesimal length increment in the -direction, corresponding to the width of the small cube.
After correcting himself, the speaker says the height is .
The final written formula is , containing .
dz
Infinitesimal length increment in the -direction, corresponding to the height of the small cube.
The speaker says, "you could call that dV, which is kind of the volume differential."
The board shows .
dV
Volume differential, the infinitesimal volume of a small rectangular box inside the larger region.
Top-left green text shows the inequality .
The speaker later says to sum in the x direction from to .
x
Cartesian coordinate along the x-axis; outer integration variable for the rectangular box.
The speaker says he wants to use the example so viewers get used to what a triple integral looks like and how it relates to a double integral.
The video uses a simple rectangular solid not because geometry is insufficient, but to build familiarity with the form of a triple integral and its relation to a double integral before moving to more complicated examples.
The region is a rectangular box with constant coordinate bounds.
The speaker says that using basic geometry one could multiply width times height times depth to get the volume.
For a rectangular solid, the volume can be found by multiplying the three side lengths corresponding to width, height, and depth.
The solid is a rectangular box with mutually perpendicular side lengths.
The speaker asks, "So what does a triple integral mean?"
In this clip, a triple integral is introduced conceptually as an object whose meaning is built from summing infinitesimal volumes inside a three-dimensional region.
The region is three-dimensional.
The explanation uses a small rectangular box as the basic volume element.
The speaker names the small volume and calls it the volume differential.
The board writes .
The infinitesimal volume element inside the large box is denoted . In Cartesian coordinates it is the product of the three side lengths of a tiny rectangular box.
Coordinates are Cartesian.
The small piece is treated as a rectangular box with side increments , , and .
The speaker assigns width , corrects height to , and assigns depth .
A small cube is drawn inside the larger dashed rectangular box.
The small cube inside the larger box has width , height , and depth , matching the three coordinate directions shown on the axes.
The cube is aligned with the coordinate axes.
The larger region is a rectangular box.
The speaker says, "you could switch the orders of these ... because multiplication is associative and order doesn't matter".
Because is written as a product of scalar differentials, the factors , , and may be reordered without changing the value of the product.
This statement concerns multiplication of the differential factors, not yet the full iterated integral setup.
The board displays dV = dx dy dz in cyan at the top right.
The speaker says to take the sum of these dVs and writes dz, dy, dx in the iterated integral.
A small cyan cube is drawn inside the larger dashed rectangular box, representing one infinitesimal piece of volume.
For a rectangular box aligned with the coordinate axes, an infinitesimal volume element is written as . In the video this element is represented by a small cube inside the larger box, and the triple integral sums such elements over the whole region.
The region is described using Cartesian coordinates.
The small volume element is rectangular, with side lengths dx, dy, and dz.
Green inequalities at top left read , , .
A dashed rectangular box is drawn in a 3D coordinate system with axes labeled x, y, and z.
The speaker uses these bounds to choose limits for z, then y, then x.
The solid region being integrated over is the rectangular box , , . The diagram shows this box in 3D space, and the inequalities give the constant limits used for each coordinate direction.
The box is axis-aligned.
All three coordinate intervals are constant and independent of the other variables.
The instructor writes an iterated integral with inner z-limits 0 to 2, then adds y-limits 0 to 4, then x-limits 0 to 3, with differentials dz dy dx.
The speaker explains that z is integrated first, y next, and x last, and that this computes the volume of the entire figure.
The final integral is not fully evaluated within the clip; the speaker only says it is straightforward to evaluate.
To compute the volume of the rectangular box, the video sets up the iterated integral . The method is to integrate first in the z-direction to get the height of a column, then sum columns in the y-direction to form a sheet, and finally sum sheets in the x-direction to obtain the total volume.
The integrand is 1, so the integral measures volume.
The limits are constant because the region is a rectangular box.
The chosen order is dz first, dy second, dx third.
Top-left bounds are , , .
Top-center formula is dV = dx dy dz.
Iterated integral is shown as \, dz \, dy \, dx.
A dashed rectangular box is drawn in a 3D coordinate system with axes labeled x, y, z.
The clip sets up the volume of a rectangular box by integrating the constant integrand 1 over the region , , . The differential order shown is dz dy dx, so the integration is performed first with respect to z, then y, then x.
The region is a rectangular box aligned with the coordinate axes.
The integrand is 1 because the goal is volume.
Speaker says, "First we're taking the integral with respect to z."
Inner evaluation is written as [z]_0^2.
Middle evaluation is written as [2y]_0^4.
Outer evaluation is written as [8x]_0^3.
The method demonstrated is to evaluate the innermost integral first, substitute its limits, carry the resulting expression outward, and repeat until only one variable remains. Each step uses the antiderivative of the current integrand with respect to the current variable.
The integral is written as an iterated integral with explicit limits.
Each integration is performed with respect to the variable indicated by the differential.
Speaker says that after integrating with respect to z, the result is a double integral and that this is the exact integral from previous videos on the double integral.
After the inner step, the board shows \, dy \, dx.
The expression is written to connect the result to a surface height.
For this rectangular box, integrating 1 with respect to z from 0 to 2 produces the constant 2. The remaining double integral \, dy \, dx matches the earlier double-integral viewpoint where the height above the xy-region is the constant function .
The upper surface is and the lower surface is .
The xy-region is and .
The speaker says integrals help us take infinite sums of infinitely small distances like , , or .
Integrals are described as tools for taking infinite sums of infinitely small quantities such as , , and .
The quantity being summed is built from infinitesimal pieces.
The setting is the volume computation introduced in this clip.
infinitely many infinitesimal pieces
The speaker says the integral as written gives the volume of a column for any x and y, and because all quantities are constant it becomes 2 times dy dx.
The inner integral shown on the board has limits to and differential dz.
For fixed x and y, the inner integral equals the height 2, so the contribution of one vertical column is .
The region has constant z-bounds .
The integrand is 1, so the integral computes volume.
x and y are held fixed while integrating with respect to z.
For any fixed x and y in the box.
The speaker says that after finding the height of a column, one can sum those columns in the y direction from to , giving the volume of a sheet parallel to the zy-plane.
A second integral sign is added with lower limit 0 and upper limit 4.
Adding the vertical columns over produces the volume of a sheet parallel to the -plane.
The previous step has already computed the height of a column in the z-direction.
The y-bound is constant from 0 to 4.
For the fixed x-slice being summed in the y-direction.
The speaker says that all that remains is to add up those sheets in the x direction from to to have the volume of the entire figure.
A third integral sign is added with lower limit 0 and upper limit 3.
The numerical value of the total volume is not stated in this clip.
Adding the sheets over yields the volume of the entire rectangular box.
The y-step has produced sheet volumes parallel to the zy-plane.
The x-bound is constant from 0 to 3.
Over the full x-interval of the box.
Speaker says, "we don't have anything written under here, but we can just assume that there's a 1" and explains that dz dy dx is the same as 1 times dz dy dx.
A red 1 is inserted before dz in the integral.
When computing volume with dV = dz dy dx and no other integrand is written, the implicit integrand is 1.
The integral is being used to compute volume.
The differential element is written without an additional function factor.
For the displayed volume integral in this clip.
Speaker says, "what we're doing with the triple integral, it's really, really nothing different" and notes that the remaining double integral is the same kind of integral discussed previously.
The speaker says he will show why triple integrals are useful "in a second," but that explanation is not contained in this clip.
In this rectangular-box example, the triple integral is presented as doing essentially the same thing as the previously discussed double integral after the z-integration is carried out.
The region is the displayed box with constant top surface .
The integral is evaluated in the order dz dy dx.
For the specific example shown in this clip.
The speaker says that if the mass was uniform, you could just multiply its uniform density times its volume and get its mass.
If a body has uniform density, then its total mass is obtained by multiplying that constant density by its volume.
The density is uniform throughout the body.
The volume of the body is known.
For a body with constant density throughout its volume.
The speaker says that when you have a constant value within the volume, you could have just done a double integral.
The statement is presented verbally as a comparison to the already-written triple integral; the clip does not fully derive the equivalence.
For computing the volume of the pictured solid, if the integrand is constant within the volume, one could have used a double integral instead of the displayed triple-integral setup.
The goal is volume rather than mass with variable density.
The integrand over the volume is constant.
In the volume-computation setting shown on the board.
The speaker says the depth is 3, the width is 4, the base area is 12, and 12 times 2 is 24 cubic units.
The drawn solid has coordinate extents matching x-length 3, y-length 4, and z-height 2.
The base area is computed from the two horizontal side lengths.
The solid is rectangular, so its base is a rectangle with side lengths 3 and 4.
The base area is multiplied by the vertical height to obtain the volume.
For a rectangular solid, volume equals base area times height.
The volume of the rectangular solid is 24 cubic units.
The speaker says the small volume equals width times length times height.
The board writes .
Start with the infinitesimal volume of the small cube inside the larger box.
The speaker explicitly introduces as the small volume differential.
Multiply the three side lengths of the small cube: depth , width , and height .
The speaker states that the volume is width times length times height and identifies those side lengths.
The volume differential for the small rectangular box is .
The speaker says they can first add the cube up in the direction to get the volume of a column.
The cursor points around the small cube and then toward the vertical -axis.
The clip ends before the actual integral notation for the column is written out.
Begin from the infinitesimal volume element of one small cube.
This was established earlier on the board.
Add copies of the small cube upward and downward along the -axis while keeping the other two dimensions fixed.
The speaker says to take the cube and add it up in the direction.
The result of that first summation is described as the volume of a column.
The speaker explicitly states that this produces the volume of a column.
The first conceptual integration direction chosen in the clip is the -direction, producing a column-like intermediate volume.
The speaker builds the integral step by step: first z from 0 to 2, then y from 0 to 4, then x from 0 to 3.
The board progressively shows nested integral signs with the corresponding limits and the differentials dz dy dx.
Start with the innermost integration in the z-direction because the smallest cube is stacked vertically from the bottom of the box to the top.
The displayed bounds include , and the speaker explicitly says to integrate with respect to z first.
After integrating in z, one vertical column has height 2 and base area dy dx, so its volume is 2 dy dx.
The speaker states that the column height is 2 and the width and depth are dy and dx.
Next, sum those columns in the y-direction to form a sheet parallel to the zy-plane.
The speaker says to take another integral in the y direction and uses the bounds to .
Finally, sum the sheets in the x-direction to obtain the volume of the whole box.
The speaker says to add up the sheets in the x direction from to .
The volume of the rectangular box is represented by the iterated triple integral .
Board shows \, dz \, dy \, dx.
Board shows [z]_0^2, then \, dy \, dx, then [2y]_0^4, then \, dx, then [8x]_0^3, then 24.
Speaker narrates each antiderivative and limit substitution, ending with "24 units cubed."
Start from the displayed iterated integral for the volume of the box.
The bounds , , and dV = dx dy dz are written on the board.
Integrate the innermost 1 with respect to z.
The antiderivative of 1 with respect to z is z, as stated by the speaker.
Evaluate [z]_{0}^{2}=2-0.
Substitute the upper and lower z-limits shown on the integral.
Integrate the middle integrand 2 with respect to y.
The antiderivative of 2 with respect to y is 2y.
Evaluate [2y]_{0}^{4}=8-0.
Substitute the y-limits 0 and 4 shown on the board.
Integrate the outer integrand 8 with respect to x.
The antiderivative of 8 with respect to x is 8x.
Evaluate [8x]_{0}^{3}=24-0.
Substitute the x-limits 0 and 3 shown on the board.
The displayed triple integral evaluates to 24 cubic units.
The board shows and the successive evaluated lines , , , , , and .
The left diagram labels the rectangular box with , , and .
Start from the iterated integral written on the board for the rectangular solid.
Observed directly from the formula on the board.
Integrate the innermost integrand with respect to .
Antiderivative of with respect to is .
Evaluate .
Substitution of the -limits shown on the board.
Integrate the middle integrand with respect to .
Antiderivative of with respect to is .
Evaluate .
Substitution of the -limits shown on the board.
Integrate the outer integrand with respect to .
Antiderivative of with respect to is .
Evaluate .
Substitution of the -limits shown on the board.
The displayed triple integral evaluates to , matching the volume of the rectangular box with side lengths , , and .
Bounds ``, ``, and `` are written on screen.
A three-dimensional rectangular solid is sketched in the first octant using those bounds.
The speaker states the goal is to find the volume of the cube/rectangular solid and later computes it as 24 cubic units.
The speaker calls the object a cube, but the displayed side lengths are 3, 4, and 2, so the mathematical object shown is a rectangular box rather than a true cube.
Given a solid bounded by , , and , determine its volume.
Compute the volume of the solid.
Record the coordinate bounds that define the solid.
These inequalities are explicitly written and spoken in the video.
Use the rectangular-solid volume formula with side lengths 3, 4, and 2.
The solid is axis-aligned with constant bounds in each coordinate direction.
Multiply the side lengths to obtain the numerical volume.
Arithmetic simplification.
24 cubic units
The result matches the speaker's verbal computation: base area 12 times height 2 gives 24.
The board lists , , and .
A dashed rectangular box is drawn in a 3D coordinate system.
Use a rectangular box in -space to explain what a triple integral means by summing tiny volume elements.
A small cube is placed somewhere inside the larger box.
Identify the infinitesimal volume element and describe the first summation direction.
The region is a rectangular box aligned with the coordinate axes.
These bounds are written directly on the board.
Inside the box, choose a tiny rectangular cube and compute its volume as the product of its three side lengths.
The speaker labels the sides , , and writes the formula on the board.
The next conceptual step is to stack these small cubes vertically to form a column.
The speaker says they can first add it up in the direction so that we get the volume of a column.
The clip sets up the volume element and begins the triple-integral interpretation by summing first along .
The written bounds, the drawn box, and the spoken explanation all match the same Cartesian volume setup.
The board lists , , and constructs the nested integral with those limits.
A dashed rectangular box in 3D coordinates is shown with a small interior cube.
The speaker explains that this integral will give the volume of the entire figure.
The clip stops before the final numerical evaluation is spoken or written.
Find the volume of the rectangular box defined by , , and using an iterated triple integral.
The region is a rectangular box in 3D Cartesian coordinates.
The coordinate bounds are , , .
The volume element is dV = dx dy dz.
Write the iterated integral that computes the volume of the box.
Use the infinitesimal volume element for a small rectangular cube inside the box.
This formula is written directly on the board.
Integrate first with respect to z from the bottom face to the top face of the box.
The speaker identifies the lowest z-value as 0 and the upper bound as 2.
Add a y-integral from 0 to 4 to sum the vertical columns into a sheet.
The speaker says y goes from 0 to 4 and describes this as summing in the y direction.
Add the outer x-integral from 0 to 3 to sum all sheets and obtain the full volume.
The speaker says to go from to to get the volume of the entire figure.
\,dy\,dx
The setup matches the displayed constant bounds , , and the stated order dz, then dy, then dx.
A dashed rectangular box is drawn in xyz-space with axis labels x, y, z.
Bounds are written as , , .
The worked integral is \, dz \, dy \, dx and the final written value is 24.
Compute the volume of the rectangular box shown in the 3D diagram using the displayed triple integral.
dV = dx dy dz
integrand is implicitly 1
Evaluate the triple integral and interpret the result as volume.
Set up the volume integral from the box bounds and volume element.
The board explicitly writes the bounds and dV = dx dy dz.
After integrating with respect to z, the inner result is 2.
[z]_0^.
After integrating with respect to y, the middle result is 8.
[2y]_0^.
After integrating with respect to x, the final numerical value is 24.
[8x]_0^.
24 cubic units
The speaker states the final result as 24 units cubed, and the board shows the final written value 24.
The board shows a rectangular solid in 3D with labeled bounds , , and .
The board shows the volume integral and later the density example with .
The speaker contrasts finding volume with finding mass when density is not uniform.
The clip sets up the mass problem but does not carry out the full triple integral for mass before it ends.
For the rectangular solid shown on the board, first compute its volume using a triple integral, then set up the corresponding mass calculation when the density is non-uniform and given by .
The solid is a rectangular box with , , and .
The volume computation on the board uses integrand .
The example density is .
The mass element is written as .
Compute the box volume and express the infinitesimal mass element for the variable-density version of the same solid.
Write the triple integral for the volume of the rectangular box.
Volume of a 3D region can be computed by integrating over the region.
Evaluate the displayed iterated integral step by step to obtain the volume.
The board explicitly shows the intermediate evaluations leading to .
Replace the constant-density/volume situation with a variable density example.
The speaker introduces a non-uniform density and writes this specific function on the board.
Express the infinitesimal mass as density times infinitesimal volume.
The speaker states that the mass of a small volume is that volume times the density at that point.
The volume of the box is . For the variable-density example, the differential mass element is .
The volume result agrees with the geometric side lengths . The mass setup follows directly from the stated rule 'small mass = density at that point times small volume.'
Green inequalities appear sequentially in the upper-left corner: first ``, then ``, then ``.
Handwritten inequalities in green
The x-bound appears first.
The y-bound is added below it.
The z-bound is added below the y-bound.
All three bounds start at 0.
Each bound is an interval along one coordinate axis.
The visual sequence defines a rectangular region in three-dimensional space by specifying independent intervals for x, y, and z.
Three green axes are drawn from a common origin and labeled x, y, and z.
x-axis
y-axis
z-axis
origin
Axes are drawn one after another.
Axis labels x, y, and z are added.
The axes share a common origin.
The sketch represents a three-dimensional coordinate system.
The coordinate frame provides the spatial setting for the solid defined by the earlier inequalities.
Tick marks are added along the axes, then dashed green edges are drawn to outline a rectangular solid in the first octant.
Exact tick placement is schematic rather than measured precisely on screen.
Rectangular solid
dashed edges
axis tick marks
Tick marks indicate the extents along each axis.
Dashed lines connect corresponding endpoints to form the box.
The top face and vertical edges are added last.
The solid remains aligned with the coordinate axes.
The lower face lies in the plane .
The side lengths correspond to the intervals 0 to 3, 0 to 4, and 0 to 2.
The animation converts the algebraic bounds into a geometric picture of the region whose volume is being discussed.
A 3D coordinate system with axes labeled , , and is shown, with a dashed rectangular box inside it.
The inequalities , , and remain visible at top left.
coordinate axes , ,
dashed rectangular box
handwritten inequalities , ,
The cursor moves around the box and axes while the drawing itself stays fixed.
The outer region remains a rectangular box.
The displayed coordinate bounds do not change.
The picture establishes a simple Cartesian solid whose volume will be built from infinitesimal sub-volumes.
A smaller solid cube is drawn inside the larger dashed box.
The speaker says, "That's my cube. It's someplace in this larger cube".
large dashed rectangular box
small solid cube inside it
A new small cube appears inside the larger region.
The speaker then labels its edges as , , and .
The small cube lies entirely within the larger box.
The coordinate axes and outer bounds remain unchanged.
The small cube represents one infinitesimal volume element used to build the triple integral.
The board writes in the upper right.
The speaker calls the volume differential.
formula
small cube diagram
The symbolic expression for the infinitesimal volume is added to the board.
The underlying geometry remains the same rectangular box with a small interior cube.
The visual formula converts the geometric side lengths of the tiny cube into the standard notation for a volume element.
The cursor points near the small cube and then toward the vertical -axis.
The speaker says they can add the cube up in the direction to get the volume of a column.
small cube
vertical -axis
cursor
Attention shifts from the small cube to the vertical direction.
No new formula is written during this interval.
The outer box and bounds remain visible.
The gesture indicates that the first summation in the triple-integral construction is taken along the -axis.
The screen shows a black digital blackboard with green inequalities at top left, cyan formula dV = dx dy dz at top right, and a 3D coordinate drawing below.
A cursor moves around the board while new integral signs and limits are written in sequence.
Top-left green inequalities for x, y, and z bounds.
Top-right cyan formula dV = dx dy dz.
Lower-left 3D coordinate axes labeled x, y, z.
Dashed rectangular box in the first octant.
Small cyan cube inside the larger box.
Nested integral signs added in cyan and pink/magenta.
First the inner z-limits 0 and 2 are written beside the first integral sign.
Then dz, dy, dx are placed to indicate the integration order.
Next a second integral sign is added with y-limits 0 and 4.
Finally a third integral sign is added with x-limits 0 and 3.
The region remains the same rectangular box throughout the clip.
The coordinate bounds listed at top left do not change.
The volume element formula dV = dx dy dz remains visible.
The visual progression turns a geometric picture of a box made of tiny cubes into an algebraic iterated integral whose nesting order mirrors successive summation in z, then y, then x.
The speaker describes first a column, then a sheet parallel to the zy-plane, then the entire figure.
The small cube inside the dashed box visually supports the idea of building larger pieces from infinitesimal volumes.
The animation does not explicitly shade a full column, sheet, or solid; these are described verbally while the static box drawing remains on screen.
One infinitesimal cube.
A vertical column obtained by summing in z.
A sheet obtained by summing in y.
The full rectangular solid obtained by summing in x.
The explanation moves from a single small cube to a vertical stack in the z-direction.
It then extends that stack across the y-interval to make a sheet.
It finally repeats that sheet across the x-interval to recover the whole box.
The box dimensions remain 3 by 4 by 2 in the x, y, z directions.
The integration order stays dz, dy, dx.
The mathematical relation being illustrated is that triple integration decomposes volume into successive one-dimensional summations: height first, then width, then depth.
A dashed rectangular box is drawn in a 3D coordinate system with axes labeled x, y, z.
Green inequalities at top left list the coordinate ranges.
Red arrows connect the written bounds to the corresponding axis directions on the box.
3D coordinate axes labeled x, y, z
dashed rectangular box
green bound inequalities
red arrows
The red 1 is added inside the integral early in the clip.
Later, intermediate antiderivatives and evaluated constants are written beneath the original integral.
Near the end, the view scrolls downward to make room for the remaining steps.
The box dimensions remain 3 by 4 by 2 throughout the clip.
The integration order remains dz dy dx once established.
The diagram visually identifies the region whose volume is being computed by the iterated integral.
Green text is written on the right side.
Speaker says the surface is and that it is a constant function independent of x and y.
The top face of the box corresponds to the plane .
box top face
expression
xy-base region
The written function appears after the inner z-integration has produced the constant 2.
The height above the xy-region stays constant at 2.
This visual connects the triple-integral computation to the earlier double-integral idea of volume under a surface.
The left half of the screen contains a green 3D coordinate sketch of a dashed rectangular box with axis labels and bound annotations; the right half contains the iterated integral and its evaluation lines.
As the clip progresses, new green handwriting is added beneath the earlier work: first , then .
3D coordinate axes
dashed rectangular box
bound labels , ,
iterated integral
evaluation lines ending at
handwritten density formula
handwritten mass-element formula
New formulas are written under the existing volume work during the second half of the clip.
The focus shifts from the already-evaluated volume integral to the newly introduced density and mass-element expressions.
The rectangular box diagram remains on screen throughout.
The previously written volume integral and its final value remain visible while the new mass setup is added.
The visual progression shows that the same solid region is being reused: first as a volume example, then as the domain for a variable-density mass calculation.
The speaker says 'find the volume of a cube' while the displayed bounds are , , and .
The three side lengths shown on screen are unequal.
The spoken wording suggests the object is a cube.
Mathematically, the displayed region is a rectangular box with side lengths 3, 4, and 2, not a cube, because a cube requires all side lengths to be equal.
The speaker first says the height is , then immediately corrects himself: "Sorry, no, its height is dz".
One might mistakenly assign the vertical height of the small cube to instead of .
In the drawing, is the up-and-down axis, so the height of the small cube is ; is the depth direction.
The speaker says he will write dz first just so it reminds us that we are going to take the integral with respect to z first, then y, then x.
One might think the differentials can be placed in any order without affecting which variable is integrated first.
In the video’s notation, writing dz first signals that the innermost integration is with respect to z, followed by y and then x.
The speaker says the result will be a function of x and y, but since all quantities here are constant it is actually a constant value.
Because an inner integral is performed while holding other variables fixed, one may expect the result always to depend on those outer variables.
Here the z-limits are constant, so after integrating in z the column volume is just the constant height 2 times dy dx, not a varying function of x and y.
Speaker explicitly addresses that nothing is written under the integral and says to assume there is a 1.
A reader might think that if no function is written inside a volume integral, there is no integrand or the integrand is unspecified in a way that prevents evaluation.
The clip states that dz dy dx is the same as 1 \, dz dy dx, so the missing integrand is 1.
Speaker says the triple integral is "really, really nothing different" and anticipates the question why do it at all.
The promised justification for why triple integrals are useful is not given within this clip.
A learner may think the triple integral introduces a wholly new computational process unrelated to double integrals.
In this example, after integrating with respect to z, the remaining computation is exactly a double integral with constant height .
The speaker says doesn't always have to be if we're doing other coordinates, mentioning polar coordinates as an example where it could be slightly different.
One might think the volume element in a triple integral is always .
In Cartesian coordinates for this box, corresponds to width times height times depth, but in other coordinate systems the expression for changes.
The speaker contrasts the uniform-density case, where mass is just density times volume, with the non-uniform case, where density changes from point to point.
One might try to compute mass by multiplying a single density value by the whole volume even when density is not uniform.
If density varies with position, mass must be built from local contributions rather than one global product.
The speaker contrasts the easy geometric method with the goal of getting used to what a triple integral looks like.
The video explicitly notes that basic geometry already solves this example, but the pedagogical purpose is to transition toward triple integrals.
The inequalities ``, ``, and `` are written first.
The later sketch uses those same extents to draw the rectangular solid.
The geometric volume formula is applied to the specific rectangular solid defined by the displayed coordinate bounds.
The speaker labels the cube sides and then writes the product formula.
appears after the side labels are discussed.
The definition of depends on first identifying the three side lengths , , and of the small cube.
After writing the product, the speaker remarks that the order can be switched because multiplication is associative and order does not matter.
The commutativity remark applies directly to the product expression defining .
The clip opens by asking what a triple integral means and later explains integrals as infinite sums of infinitesimal pieces.
The infinitesimal piece used here is .
The conceptual meaning of the triple integral in this clip contains the construction of the volume element as the basic summed piece.
After defining , the speaker says they can first add it up in the direction to get a column.
The volume element is the object being summed in the first integration step along .
The board shows dV = dx dy dz and then builds an integral summing such elements.
The speaker refers to taking the sum of these dVs when setting up the integral.
The differential volume element dV = dx dy dz is the basic piece being summed by the triple integral setup.
The inequalities , , are used directly as the limits of the nested integrals.
The speaker chooses the z, y, and x limits from these displayed inequalities.
The constant coordinate bounds of the rectangular box determine the limits of each iterated integral.
The speaker says the inner integral gives the volume of a column and equals 2 dy dx.
The innermost integral shown is from to with dz.
The geometric interpretation of a vertical column depends on evaluating the inner z-integral first.
The speaker first forms a sheet by summing in y, then obtains the whole figure by summing in x.
Additional integral signs are nested outside the earlier ones with y-limits 0 to 4 and x-limits 0 to 3.
The full solid volume is obtained by generalizing the sheet construction across the remaining x-direction.
The bounds and dV are written first, then the iterated evaluation proceeds step by step.
The rectangular-box setup is evaluated using the inside-out iterated integration method.
Speaker says the result after the z-step is a double integral and compares it to previous double-integral videos.
The board shows \, dy \, dx after the inner step.
The triple-integral evaluation contains a stage that is precisely a double integral over the xy-region with constant height 2.
The three inequalities defining the region are visible on screen.
The speaker explains that the example is meant to introduce triple integrals and their relation to double integrals.
The speaker computes 12 times 2 to get 24 cubic units.
The speaker asks, "So what does a triple integral mean?"
The board shows .
The speaker describes it as width times length times height.
The speaker says the order can be switched because multiplication is associative and order does not matter.
The speaker says they can first add the cube up in the direction to get the volume of a column.
The speaker corrects the height label from to .
Top-right formula reads dV = dx dy dz.
The speaker talks about summing these dVs.
The speaker says he writes dz first to remind us that the integral is taken with respect to z first.
The innermost integral has limits to .
The displayed bounds are , , .
The speaker uses these exact numbers as the limits of the nested integrals.
The speaker describes a column, then a sheet parallel to the zy-plane, then the entire figure.
A small cube inside a larger dashed box illustrates the buildup.
Covered · Opening black screen transitions into the spoken setup of the volume problem.
Covered · The coordinate bounds , , and are written and read aloud.
Covered · The speaker notes that geometry would suffice and states the pedagogical aim of introducing triple integrals.
Covered · A three-dimensional coordinate system is drawn and the rectangular solid is sketched from the given bounds.
Covered · The speaker computes the volume geometrically as 24 cubic units and begins transitioning toward the integral approach.
Covered · Opening question about the meaning of a triple integral.
Covered · Speaker motivates taking the volume of a very small volume inside the region.
Covered · A small cube is drawn and its side lengths are identified as , , and .
Covered · The formula is written and discussed.
Covered · The speaker explains integrals as infinite sums of infinitesimal distances.
Covered · The first summation direction is chosen as the -direction to form a column.
Covered · Initial board state and construction of the inner z-integral with dz dy dx order.
Covered · Explanation that the inner integral gives the volume of one vertical column, equal to 2 dy dx.
Covered · Addition of the y-integral from 0 to 4 and interpretation as forming a sheet parallel to the zy-plane.
Covered · Addition of the x-integral from 0 to 3 to obtain the full volume setup; evaluation is announced but not performed.
Covered · The box, bounds, dV = dx dy dz, and implicit integrand 1 are introduced.
Covered · The inner z-integration is evaluated to 2 and rewritten as a double integral.
Covered · The speaker connects the remaining double integral to and says the triple integral is not fundamentally different here.
Covered · The y- and x-integrations are completed, yielding 24 cubic units.
Covered · Audio contrasts constant-integrand volume computation with the new goal of finding mass; the board already shows the box and the volume integral.
Covered · The speaker explains uniform versus non-uniform density and motivates a variable density function.
Covered · The density symbol is introduced and the example is written on the board.
Covered · The speaker defines the small-mass element as density times small volume and writes .
Covered · The speaker interprets as width times height times depth in Cartesian coordinates and warns that other coordinate systems change its form.
Covered · No additional distinct mathematical content is introduced in the final fraction of the clip beyond the ongoing explanation of .
Covered · All mathematical content in the video has been covered.
Reviewed subject paths