Why Polar Bonds Can Form a Nonpolar Molecule
A molecule can contain polar covalent bonds yet have no overall dipole. Learn how molecular shape, electronegativity, and bond dipole cancellation determine molecular polarity, using CO₂, H₂O, HCN, and other examples.
A carbon dioxide molecule contains two polar covalent bonds. Oxygen attracts the shared electrons more strongly than carbon, so each C=O bond has an uneven distribution of electron density.
Yet carbon dioxide, \(\ce{CO2}\), is a nonpolar molecule.
That seems contradictory. If both bonds are polar, shouldn’t the whole molecule be polar?
No. Bond polarity describes what happens within an individual bond. Molecular polarity describes the overall distribution of charge across the entire molecule. In carbon dioxide, the two equal bond dipoles point in opposite directions and cancel.
This is the central idea: a molecule can contain polar bonds but have no overall permanent dipole because of its three-dimensional shape and the directions of its bond dipoles.
01Bond polarity and molecular polarity are different
Start by imagining two people pulling a trolley with equal force in opposite directions.
Both people are pulling. Neither force disappears. But the trolley experiences no net force because the two pulls cancel.
Bond dipoles behave similarly when we add them as vectors.
A vector has both magnitude and direction. Two equal vectors pointing in opposite directions produce a resultant of zero.
The analogy is useful for understanding cancellation, although bond dipoles are not mechanical forces. They describe the distribution of electrical charge within a molecule.
What makes a covalent bond polar?
A covalent bond forms when atoms share electrons.
However, the electrons are not always shared equally.
Consider a carbon-oxygen bond. Oxygen is more electronegative than carbon, meaning it attracts the shared bonding electrons more strongly.
As a result:
- Oxygen develops a partial negative charge, written \(\delta-\).
- Carbon develops a partial positive charge, written \(\delta+\).
These are partial charges, not full ionic charges.
A bond with this uneven electron distribution is called a polar covalent bond.
We represent its polarity using a bond dipole arrow. In the chemistry convention, the arrow points towards the more electronegative atom, which is the partially negative end. A small cross marks the partially positive end.
What makes an entire molecule polar?
Now consider the molecule as a whole.
Each polar bond contributes a bond dipole. These dipoles have different directions depending on the three-dimensional arrangement of the atoms.
The overall molecular dipole is determined by adding the individual contributions as vectors.
There are three possibilities:
| Arrangement of bond dipoles | Result |
|---|---|
| Equal dipoles in opposite directions | They cancel. |
| Dipoles pointing in the same direction | They reinforce each other. |
| Dipoles pointing in different directions | They may partially cancel, leaving a resultant. |
A molecule is nonpolar when its permanent molecular dipole moment is zero.
A molecule is polar when it has a nonzero permanent molecular dipole moment.
Notice that the number of polar bonds alone cannot tell you whether a molecule is polar.
02Why carbon dioxide is nonpolar despite its polar bonds
Carbon dioxide is the clearest example of this idea.
First, establish its electron arrangement.
Carbon is in Group 14 and contributes four valence electrons. Each oxygen is in Group 16 and contributes six.
The total number of valence electrons is:
\[
4+2(6)=16
\]
A suitable Lewis structure is:
\[
\ce{O=C=O}
\]
Each oxygen has two lone pairs, while carbon has no lone pairs.
The formal charges on all three atoms are zero.
However, this does not mean the C=O bonds are nonpolar.
Formal charges and partial charges describe different things:
- Formal charge is an electron-bookkeeping calculation based on an assumed equal division of shared electrons.
- Partial charge describes the actual uneven distribution of electron density.
Because oxygen is more electronegative than carbon, both oxygen atoms have a partial negative character, while carbon has a partial positive character.
The importance of molecular shape
Carbon dioxide has two electron regions around its central carbon atom. Each double bond counts as one electron region.
With no lone pairs on carbon, the molecule is linear.
Its O-C-O bond angle is \(180^\circ\).
Now consider the two bond dipoles.
- The left C=O bond dipole points towards the left oxygen.
- The right C=O bond dipole points towards the right oxygen.
- Both dipoles have the same magnitude because the two C=O bonds are equivalent.
- Their directions are exactly opposite.
Therefore, they cancel completely.
\[
\vec{\mu}_{\mathrm{net}}
=
\vec{\mu}_1+\vec{\mu}_2
=
0
\]
The molecule has no permanent dipole moment.
The important point is that the C=O bonds remain polar. Their individual polarities have not disappeared. Their combined effect is simply zero.
What if the molecule were bent instead?
Imagine changing the arrangement so that the two oxygen atoms were no longer directly opposite each other.
The bond dipoles would no longer point in opposite directions. Some components would cancel, but a component would remain along the angle bisector.
This is exactly what happens in water, \(\ce{H2O}\).
Oxygen forms two polar O-H bonds and has two lone pairs. The molecule is bent, with an H-O-H bond angle of approximately \(104.5^\circ\).
The two bond dipoles therefore cannot cancel.
Water has a permanent molecular dipole moment of approximately \(1.85\ \mathrm{D}\), where D stands for Debye, a unit of dipole moment.
This comparison gives you a useful prediction:
- Linear molecules with identical terminal atoms and equivalent bonds can have complete dipole cancellation.
- Bent molecules with two equivalent polar bonds generally have a nonzero resultant.
But be careful. Linear geometry does not automatically mean a molecule is nonpolar.
We will see why shortly.
03Why the Lewis structure alone cannot tell you molecular polarity
A common mistake is to look at a Lewis structure and decide that the molecule is nonpolar because the drawing looks balanced.
A Lewis structure is not necessarily a picture of the molecule’s actual three-dimensional arrangement.
Different representations communicate different information.
| Representation | What it tells you | What it does not establish |
|---|---|---|
| Molecular formula | Which atoms are present and their numbers | Molecular shape |
| Lewis structure | Bonds, lone pairs, valence electrons, and formal charges | Exact three-dimensional arrangement |
| Molecular shape model | Relative positions of atoms in space | Complete electron distribution |
| Bond dipole arrows | Direction and approximate relative magnitude of bond polarities | Exact molecular dipole moment |
| Experimental dipole measurement | Whether a permanent molecular dipole exists and its magnitude | A complete Lewis structure |
This is why you should establish the molecular shape before deciding whether the molecule is polar.
If you need to refresh how to count valence electrons and construct Lewis structures, see Lewis Dot Diagrams for Atoms, Ions and Covalent Molecules.
For a more detailed explanation of electron-pair geometry and molecular shape, see Electron-Pair Geometry vs Molecular Shape: HSC Chemistry.
A useful contrast: two linear molecules
Consider carbon dioxide and hydrogen cyanide, \(\ce{HCN}\).
Both molecules are linear.
However, only carbon dioxide is nonpolar.
In carbon dioxide, the two terminal oxygen atoms are identical. The C=O bond dipoles have equal magnitudes and point in opposite directions.
Hydrogen cyanide has a different arrangement:
\[
\ce{H-C\bond{#}N}
\]
Carbon is more electronegative than hydrogen, while nitrogen is more electronegative than carbon.
Therefore:
- The H-C bond dipole points towards carbon.
- The C-N bond dipole points towards nitrogen.
Both arrows point along the same overall direction, towards nitrogen.
Instead of cancelling, their contributions reinforce each other.
This gives us an important correction to the simple rule about linear molecules.
A linear molecule is nonpolar only when its charge distribution is sufficiently symmetrical for the dipole contributions to cancel.
Being linear is not enough.
04Lone pairs can also influence molecular polarity
So far, we have focused on the directions of bond dipoles.
However, lone pairs also matter because they influence molecular shape and contribute to the overall distribution of electron density.
Consider ammonia, \(\ce{NH3}\), and nitrogen trifluoride, \(\ce{NF3}\).
Both molecules have:
- Three covalent bonds around nitrogen.
- One lone pair on nitrogen.
- A trigonal pyramidal molecular shape.
You might predict that \(\ce{NF3}\) is more polar because fluorine is more electronegative than hydrogen.
That prediction seems reasonable. Each N-F bond is more polar than an N-H bond.
But the overall result is the opposite.
Approximate experimental gas-phase dipole moments are:
| Molecule | Molecular dipole moment |
|---|---|
| \(\ce{NH3}\) | \(1.47\ \mathrm{D}\) |
| \(\ce{NF3}\) | \(0.24\ \mathrm{D}\) |
Why is ammonia so much more polar?
In ammonia, nitrogen is more electronegative than hydrogen. The three N-H bond dipoles point towards nitrogen.
Their combined contribution reinforces the charge separation associated with the electron-rich lone-pair region.
In nitrogen trifluoride, fluorine is more electronegative than nitrogen. The three N-F bond dipoles point away from nitrogen and towards fluorine.
Their resultant therefore opposes the contribution associated with the lone-pair electron density.
The two effects partially cancel, leaving a much smaller molecular dipole.
Notice something important: \(\ce{NF3}\) is still polar. Its dipole moment is small, but it is not zero.
Also, a lone pair is not literally another covalent bond dipole. Treating it as a separate contribution is a simplified way to describe the overall electron distribution.
For most HSC questions, start with bond polarity and molecular geometry. Recognise that lone-pair electron density can also matter when explaining measured molecular dipoles.
05How do chemists measure whether a molecule is polar?
So far, we have predicted molecular polarity using electronegativity, Lewis structures, and molecular shape.
But how do we know that these predictions describe real molecules?
One experimental method is microwave rotational spectroscopy.
It provides physical evidence for permanent molecular dipoles by measuring how gas molecules interact with microwave radiation.
The experimental arrangement
Imagine a low-pressure gas sample inside a narrow cell.
A tunable microwave source is connected to one end of the cell. The microwave radiation travels through the gas and reaches a detector at the other end.
Two metal electrodes sit on opposite sides of the cell. They can produce a controlled electric field through the sample.
The apparatus therefore contains four main components:
- A microwave source that produces radiation at adjustable frequencies.
- A low-pressure gas cell containing the molecules being investigated.
- Electrodes that apply an external electric field.
- A detector that measures the microwave radiation passing through the cell.
What should the experiment show?
Molecules can rotate.
However, molecular rotation is quantised, meaning molecules can only occupy particular rotational energy levels.
When microwave radiation has the correct frequency, a molecule with a permanent dipole can absorb energy and move between rotational states.
The detector records this absorption as a peak in the microwave spectrum.
Now consider what happens when the external electric field is switched on.
A permanent molecular dipole interacts with the applied field. This changes the rotational energy levels, causing characteristic shifts or splittings in the observed spectral lines.
This field-dependent change is called the Stark effect.
The presence and pattern of these changes provide evidence for a permanent molecular dipole.
Comparing carbon dioxide and water
Consider the predictions for two gas samples.
| Observation | Carbon dioxide | Water |
|---|---|---|
| Polar covalent bonds | Yes | Yes |
| Permanent molecular dipole | No | Yes |
| Ordinary pure rotational microwave absorption | No | Yes |
| Permanent-dipole Stark response | No | Yes |
The absence of an ordinary pure rotational electric-dipole spectrum for \(\ce{CO2}\) is consistent with its zero permanent dipole moment.
Water, by contrast, has a permanent dipole and produces rotational microwave absorption.
This is experimental support for the idea that the two O-H bond dipoles in water do not cancel, while the two C=O bond dipoles in carbon dioxide do.
For a more advanced explanation of the rotational selection rules, see Chemistry LibreTexts’ overview of microwave rotational spectroscopy.
Why a simple electric-field test is not enough
You might suggest a simpler experiment.
Send molecules through a non-uniform electric field and see whether they are deflected.
A polar molecule can experience a force in a field gradient because its permanent dipole interacts with the field.
But there is a problem.
Even a nonpolar molecule can have its electron cloud distorted by an external electric field. This produces an induced dipole.
The molecule can then be attracted towards the stronger-field region.
This means that observing deflection alone does not prove that a molecule has a permanent dipole.
The improved experimental approach uses rotational microwave absorption and examines the response to a controlled electric field. It distinguishes the permanent-dipole behaviour from the response caused by polarisation of the electron cloud.
There are also limits to the spectroscopy result:
- The sample must have suitable pressure and temperature.
- The instrument must cover the relevant frequency range.
- The detector must be sensitive enough to identify the absorption lines.
- The absence of a pure rotational microwave spectrum does not mean the molecule cannot be detected using other techniques.
For example, carbon dioxide can absorb infrared radiation during vibrations that change its dipole moment, even though its equilibrium structure has no permanent dipole.
The experiment measures physical behaviour. It does not photograph electrons or directly display a Lewis structure.
06Worked examples
Worked example: Estimate the partial charge in hydrogen chloride
Gas-phase hydrogen chloride, \(\ce{HCl}\), has an experimentally measured dipole moment of \(1.1085\ \mathrm{D}\) and an equilibrium bond length of \(1.27455\ \text{Å}\).
Estimate the effective partial charge on each atom using a simple two-point-charge model.
Use:
- \(1\ \mathrm{D}=3.33564\times10^{-30}\ \mathrm{C\,m}\)
- \(1\ \text{Å}=10^{-10}\ \mathrm{m}\)
- Elementary charge, \(e=1.602\times10^{-19}\ \mathrm{C}\)
The molecular data are available from the NIST Chemistry WebBook.
Step 1
For two opposite point charges, the magnitude of the dipole moment is:
\[
\mu=qr
\]
where:
- \(\mu\) is the dipole moment in \(\mathrm{C\,m}\).
- \(q\) is the magnitude of the separated charge in coulombs.
- \(r\) is the distance between the charges in metres.
Rearrange to make \(q\) the subject:
\[
q=\frac{\mu}{r}
\]
Step 2
\[
\begin{aligned}
\mu&=1.1085(3.33564\times10^{-30})\\
&=3.6976\times10^{-30}\ \mathrm{C\,m}
\end{aligned}
\]
Step 3
\[
r=1.27455\times10^{-10}\ \mathrm{m}
\]
Step 4
\[
\begin{aligned}
q&=\frac{3.6976\times10^{-30}}
{1.27455\times10^{-10}}\\
&=2.90\times10^{-20}\ \mathrm{C}
\end{aligned}
\]
Step 5
\[
\begin{aligned}
\frac{q}{e}
&=\frac{2.90\times10^{-20}}
{1.602\times10^{-19}}\\
&=0.181
\end{aligned}
\]
The effective partial charges are therefore approximately:
\[
\mathrm{H}^{0.181+}
\qquad
\mathrm{Cl}^{0.181-}
\]
The calculation shows that the effective charge separation is approximately \(0.18e\).
This does not mean that exactly \(0.18\) of an electron has been transferred from hydrogen to chlorine. The electron distribution is continuous, and the two-point-charge model is an approximation.
It does, however, demonstrate how a measured molecular dipole moment provides information about the separation of electrical charge.
Worked example: Calculate the molecular dipole of a bent molecule
An idealised molecule \(\ce{XY2}\) has two identical polar X-Y bonds.
Each bond has a dipole moment of \(1.2\ \mathrm{D}\), and the Y-X-Y bond angle is \(120^\circ\).
Calculate the magnitude and direction of the resultant molecular dipole using the bond-dipole model.
Step 1
Both bond dipoles are \(1.2\ \mathrm{D}\).
Because the molecule is symmetrical, the components perpendicular to the angle bisector cancel.
The components along the angle bisector reinforce each other.
Step 2
The angle between each bond dipole and the bisector is:
\[
\frac{120^\circ}{2}=60^\circ
\]
The component of each bond dipole along the bisector is:
\[
1.2\cos60^\circ=0.6\ \mathrm{D}
\]
Step 3
\[
\begin{aligned}
\mu_{\mathrm{net}}
&=2\mu_b\cos\left(\frac{\theta}{2}\right)\\
&=2(1.2)\cos60^\circ\\
&=1.2\ \mathrm{D}
\end{aligned}
\]
Step 4
The resultant points along the angle bisector towards the two Y atoms.
The molecule is therefore polar, with a resultant dipole moment of \(1.2\ \mathrm{D}\).
Compare this with carbon dioxide. If the angle were \(180^\circ\), the two equal bond dipoles would point in opposite directions and the resultant would be zero.
This example uses a simplified bond-dipole model. An actual molecular dipole depends on the complete electron and nuclear charge distribution, including contributions not represented by individual bond arrows.
07A reliable method for deciding whether a molecule is polar
When you encounter an unfamiliar covalent molecule in an HSC question, use the following sequence.
1. Construct or check the Lewis structure.
Count the total valence electrons, account for any overall charge, and identify the bonds and lone pairs.
2. Determine the three-dimensional molecular shape.
Do not assume the molecule is flat just because its Lewis structure is drawn on a flat page.
3. Identify the polar bonds.
Use electronegativity differences to determine which bonds have unequal electron sharing.
4. Draw the bond dipole arrows.
Use the chemistry convention: arrows point towards the more electronegative atoms.
5. Add the dipoles as vectors.
Check whether the dipoles cancel, reinforce each other, or partially cancel.
6. State the overall molecular polarity.
A zero resultant means the molecule has no permanent dipole. A nonzero resultant means it is polar.
One final check is particularly useful:
- Symmetrical molecules with identical terminal atoms and equivalent bonds often have zero net dipole.
- Molecules with different terminal atoms may be polar even when their geometry is symmetrical.
- Lone pairs can change molecular shape and contribute to the overall electron distribution.
The word to remember is symmetry. You are looking for symmetry in the distribution of charge, not simply a molecule that looks balanced on a page.
08Questions and solutions
Question 1
Carbon dioxide, \(\ce{CO2}\), contains two C=O double bonds.
Oxygen is more electronegative than carbon, and the molecule has a linear shape with an O-C-O bond angle of \(180^\circ\).
Explain why carbon dioxide is nonpolar despite containing two polar covalent bonds.
Your answer should refer to bond polarity, molecular geometry, and the resultant dipole moment.
Solution 1
Carbon dioxide is nonpolar because its two equal C=O bond dipoles point in opposite directions and cancel completely.
Oxygen is more electronegative than carbon, so each C=O bond is polar. The oxygen atom attracts the shared electrons more strongly, producing a partial negative charge on oxygen and a partial positive charge on carbon.
The molecule is linear, with a bond angle of \(180^\circ\).
The two C=O bonds are equivalent, so their bond dipoles have equal magnitudes.
When the vectors are added:
\[
\vec{\mu}_{\mathrm{net}}
=
\vec{\mu}_1+\vec{\mu}_2
=
0
\]
Therefore, carbon dioxide has no permanent molecular dipole.
The tempting mistake is to assume that two polar bonds must produce a polar molecule. This ignores the directions of the bond dipoles.
The correct conclusion is that polar bonds can exist within a nonpolar molecule when their dipole contributions cancel.
Question 2
Two unknown gases, P and Q, are investigated using microwave rotational spectroscopy.
The apparatus contains a low-pressure gas cell, a tunable microwave source, a detector, and electrodes that can apply an external electric field.
The following observations are recorded:
| Observation | Gas P | Gas Q |
|---|---|---|
| Pure rotational microwave absorption | Present | Not detected |
| Spectral response when an electric field is applied | Characteristic line shifts | No detectable permanent-dipole response |
| Deflection in a non-uniform electric field | Yes | Yes |
An HCl calibration sample produces the expected microwave absorption lines. Assume the scan covers the allowed rotational transitions and the instrument has adequate sensitivity.
Independent structural evidence indicates that both gases contain polar covalent bonds.
A student concludes that gas Q must also have a permanent molecular dipole because it is deflected by the non-uniform electric field.
Evaluate the student’s conclusion. Explain what the experimental evidence suggests about P and Q, and why the two field-based observations are not contradictory.
Solution 2
Gas P has a permanent molecular dipole, while gas Q has no detectable permanent dipole under the stated experimental conditions.
The two observations involving the electric field are not contradictory because they test different electrical responses.
For gas P, the microwave radiation produces rotational absorption lines. When the external electric field is applied, the lines shift in a characteristic way.
This supports the presence of a permanent molecular dipole. The dipole interacts with the electric field, changing the rotational energy levels.
Gas Q behaves differently.
It produces no detectable ordinary pure rotational electric-dipole absorption under the stated conditions. This supports the conclusion that its permanent molecular dipole is zero or below the experimental detection limit.
However, gas Q can still be deflected in a non-uniform electric field.
Its electron cloud can be distorted by the external field, creating an induced dipole. This induced dipole interacts with the field gradient and can cause the molecule to move towards the stronger-field region.
Therefore, deflection does not necessarily demonstrate permanent molecular polarity.
The independent evidence that Q contains polar covalent bonds is entirely consistent with this result. Its individual bond dipoles can cancel across the molecule, just as they do in carbon dioxide.
The important distinction is between a permanent dipole, which exists without an external field, and an induced dipole, which develops in response to an external field.
Question 3
Hydrogen cyanide, \(\ce{HCN}\), and carbon dioxide, \(\ce{CO2}\), are both linear molecules.
A student argues:
“Both molecules are linear, so their bond dipoles must cancel. Therefore, both molecules are nonpolar.”
Evaluate this statement.
Use electronegativity differences and the directions of the bond dipoles to explain the polarity of each molecule.
Solution 3
The student’s statement is incorrect. Carbon dioxide is nonpolar, but hydrogen cyanide is polar.
The reason is that linear geometry alone does not guarantee dipole cancellation.
For carbon dioxide:
- Oxygen is more electronegative than carbon.
- Both C=O bond dipoles point away from the central carbon towards oxygen.
- The two dipoles have equal magnitudes.
- They point in opposite directions along the same straight line.
Their resultant is zero.
For hydrogen cyanide:
- Carbon is more electronegative than hydrogen.
- Nitrogen is more electronegative than carbon.
- The H-C bond dipole points towards carbon.
- The C-N bond dipole points towards nitrogen.
Because the atoms are arranged H-C-N in a straight line, both bond dipole arrows point towards the nitrogen end.
They reinforce rather than cancel.
Therefore, \(\ce{HCN}\) has a nonzero permanent dipole moment and is polar.
The misconception is confusing molecular geometry with molecular symmetry. Both molecules are linear, but only carbon dioxide has equivalent terminal atoms and equal, opposite bond dipoles.
Question 4
Ammonia, \(\ce{NH3}\), and nitrogen trifluoride, \(\ce{NF3}\), both have trigonal pyramidal molecular shapes.
Each molecule contains three polar covalent bonds and one lone pair on nitrogen.
Approximate experimental gas-phase dipole moments are:
| Molecule | Molecular dipole moment |
|---|---|
| \(\ce{NH3}\) | \(1.47\ \mathrm{D}\) |
| \(\ce{NF3}\) | \(0.24\ \mathrm{D}\) |
A student argues that nitrogen trifluoride should be more polar because fluorine is more electronegative than hydrogen.
Explain why the experimental results contradict this prediction.
Your answer should discuss bond dipole directions, the lone-pair electron distribution, and the overall molecular dipole.
Solution 4
Ammonia has a much larger molecular dipole moment than nitrogen trifluoride, even though N-F bonds are more polar than N-H bonds.
The difference comes from the relative directions of the bond dipoles and the contribution of the lone-pair electron distribution.
In ammonia, nitrogen is more electronegative than hydrogen.
Each N-H bond dipole points towards nitrogen. The resultant of the three bond dipoles reinforces the charge separation associated with the lone-pair region on nitrogen.
The contributions therefore reinforce one another, producing a relatively large molecular dipole.
In nitrogen trifluoride, fluorine is more electronegative than nitrogen.
Each N-F bond dipole points towards fluorine. The resultant of the three bond dipoles therefore points away from the nitrogen atom.
This opposes the contribution associated with the electron-rich lone-pair region on nitrogen.
The two contributions partially cancel, leaving a much smaller molecular dipole.
Nitrogen trifluoride is still polar because the cancellation is incomplete.
The student’s mistake was assuming that greater bond polarity must produce greater molecular polarity. Molecular polarity depends on the complete charge distribution, not just the electronegativity difference of an individual bond.
Question 5
Consider a hypothetical molecule \(\ce{AX3Y}\).
The central atom A is surrounded by four atoms in an ideal tetrahedral arrangement.
The supplied bond-dipole data are:
| Bond | Bond dipole magnitude |
|---|---|
| Each of the three A-X bonds | \(1.0\ \mathrm{D}\) |
| The A-Y bond | \(2.0\ \mathrm{D}\) |
Assume:
- All four bond dipole arrows point from A towards their respective terminal atoms.
- The tetrahedral bond angles are exactly \(109.5^\circ\).
- The supplied dipole magnitudes are model values.
- The geometry is ideal and is not distorted by the different terminal atoms.
A student argues:
“The molecule is tetrahedral, so the four bond dipoles must cancel. Its molecular dipole moment is zero.”
Determine whether this conclusion is correct.
Calculate the magnitude and direction of the resultant molecular dipole. Explain why the symmetry of a tetrahedral arrangement does not guarantee cancellation in this case.
Solution 5
The student’s conclusion is incorrect. The molecule is polar, with a resultant dipole moment of \(1.0\ \mathrm{D}\) directed towards Y.
The key is that tetrahedral geometry only guarantees complete cancellation when the four bond dipole vectors have equal magnitudes and are arranged symmetrically.
Here, the A-Y bond dipole is twice as large as each A-X bond dipole.
We can establish the resultant using the geometry of a regular tetrahedron.
Step 1: Consider the direction of the A-Y bond dipole.
Take the A-Y bond direction as the positive reference direction.
Its dipole magnitude is:
\[
\mu_Y=2.0\ \mathrm{D}
\]
Step 2: Resolve the three A-X bond dipoles along the A-Y direction.
Each A-X bond makes an angle of \(109.5^\circ\) with the A-Y bond.
The component of each A-X dipole along the A-Y direction is:
\[
\begin{aligned}
\mu_{X,\parallel}
&=1.0\cos109.5^\circ\\
&\approx-0.333\ \mathrm{D}
\end{aligned}
\]
The negative sign indicates that each component points opposite to the A-Y direction.
Step 3: Add the three A-X components.
The three X atoms are symmetrically arranged around the A-Y axis.
Their components perpendicular to this axis cancel one another.
Their parallel components add:
\[
\begin{aligned}
\mu_{X,\mathrm{resultant}}
&=3(-0.333)\\
&\approx-1.0\ \mathrm{D}
\end{aligned}
\]
Therefore, the combined effect of the three A-X bond dipoles is a \(1.0\ \mathrm{D}\) resultant pointing opposite to the A-Y direction.
Step 4: Add the A-Y dipole.
The A-Y bond contributes \(+2.0\ \mathrm{D}\).
The three A-X bonds contribute approximately \(-1.0\ \mathrm{D}\).
Therefore:
\[
\begin{aligned}
\mu_{\mathrm{net}}
&=2.0-1.0\\
&=1.0\ \mathrm{D}
\end{aligned}
\]
The resultant points towards Y.
Why was the student’s prediction tempting?
Tetrahedral molecules such as \(\ce{CF4}\) are nonpolar because their four equivalent C-F bond dipoles cancel.
However, this cancellation relies on all four bond dipoles having equal magnitudes and equivalent spatial positions.
In \(\ce{AX3Y}\), the A-Y bond dipole is stronger than the other three. The three A-X dipoles combine to oppose it, but they cannot completely cancel it.
If all four bond dipoles had magnitude \(1.0\ \mathrm{D}\), the resultant would indeed be zero.
The decisive condition is therefore not simply tetrahedral geometry. It is the combination of geometry, bond equivalence, and dipole magnitude.
This is why you should never classify a molecule as nonpolar using its shape alone.
09Where to go next
Once you can determine whether a molecule has a permanent dipole, you can use that information to predict its intermolecular attractions.
Polar molecules can experience dipole-dipole attractions, while all molecules experience London dispersion forces. Some molecules can also form hydrogen bonds under the appropriate structural conditions.
The next step is connecting molecular polarity to intermolecular forces and explaining how these attractions influence boiling points, melting points, and other physical properties.