Skip to main content

Registration is now open for this year's LibreFest! Join us virtually the week of July 13.

Register here
Chemistry LibreTexts

14.6: ¹H NMR Signal Integration and Splitting

  • Page ID
    501142
  • \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)

    \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)

    \( \newcommand{\dsum}{\displaystyle\sum\limits} \)

    \( \newcommand{\dint}{\displaystyle\int\limits} \)

    \( \newcommand{\dlim}{\displaystyle\lim\limits} \)

    \( \newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\)

    ( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\)

    \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)

    \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\)

    \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)

    \( \newcommand{\Span}{\mathrm{span}}\)

    \( \newcommand{\id}{\mathrm{id}}\)

    \( \newcommand{\Span}{\mathrm{span}}\)

    \( \newcommand{\kernel}{\mathrm{null}\,}\)

    \( \newcommand{\range}{\mathrm{range}\,}\)

    \( \newcommand{\RealPart}{\mathrm{Re}}\)

    \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)

    \( \newcommand{\Argument}{\mathrm{Arg}}\)

    \( \newcommand{\norm}[1]{\| #1 \|}\)

    \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)

    \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\AA}{\unicode[.8,0]{x212B}}\)

    \( \newcommand{\vectorA}[1]{\vec{#1}}      % arrow\)

    \( \newcommand{\vectorAt}[1]{\vec{\text{#1}}}      % arrow\)

    \( \newcommand{\vectorB}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)

    \( \newcommand{\vectorC}[1]{\textbf{#1}} \)

    \( \newcommand{\vectorD}[1]{\overrightarrow{#1}} \)

    \( \newcommand{\vectorDt}[1]{\overrightarrow{\text{#1}}} \)

    \( \newcommand{\vectE}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{\mathbf {#1}}}} \)

    \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)

    \(\newcommand{\longvect}{\overrightarrow}\)

    \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)

    \(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)

    Integration of Signal Areas

    Signal integration in NMR (Nuclear Magnetic Resonance) spectroscopy is crucial for quantifying the relative number of nuclei contributing to each signal in the spectrum. This process involves measuring the area under each peak in the NMR spectrum, which directly correlates to the abundance of the corresponding nuclei in the sample.

    The computer in the NMR instrument can be instructed to mathematically integrate the area under a signal or group of signals. The signal integration process is very useful in 1H NMR spectrum, because the area under a signal is proportional to the number of protons to which the signal corresponds.

    As an example, methyl acetate, the Ha and Hb peaks would integrate to approximately the same area, because they both correspond to a set of three equivalent protons.

    Lewis structure of methyl acetate with the two groups of hydrogens labeled as A and B and colored in red and blue.

    Now, take a look at the spectrum of para-xylene (IUPAC name 1,4-dimethylbenzene). The Figure \(\PageIndex{1}\) is the 1H NMR spectrum of 1,4-dimethylbenzene with integration line (blue lines). The integration line generated by the computer is always in a curved shape that resembles steps. The integration numbers are also generated by the computer together with the curve, which shows the relative area of each signal.

    Infrared spectrum for 1,4-dimethylbenzene. HA has a pear around 2.6 ppm and  HB has a peak around 7.4 ppm.
    Figure \(\PageIndex{1}\): The 1H NMR spectrum of 1,4-dimethylbenzene with integration

     

    As we discussed earlier, the molecule of 1,4-dimethylbenzene has two sets of equivalent protons: the four aromatic (Ha) protons and the six methyl (Hb) protons. The integration of the area under the peak at 2.6 ppm is 1.5 times greater than the area under the peak at 7.4 ppm. Please note that the integration number show the relative ratio of the number of protons, not the actual number. The ratio 1.5 to 1 here matches the ratio of the actual numbers 6 to 4. This integration information, along with the chemical shift knowledge we have learned before, allows us to assign the peaks: the peak at 7.4 ppm corresponds to protons (Ha) on the benzene ring, and the peak at 2.6 ppm corresponds to two methyl groups (Hb).

     

     

    Signal Splitting (Coupling)

    In the 1H NMR spectra that we have seen so far, each set of protons generates a single NMR signal. This is not that common for 1HNMR actually. In fact, the 1H NMR spectra of most organic molecules contain signals that are ‘split’ into two or more peaks, which is called splitting (or coupling). The spectra with peak splitting may look more complicated; however, this splitting behavior provides very useful information about the structure of a compound.

    Let’s consider the spectrum for 1,1,2-trichloroethane (Figure \(\PageIndex{2}\)). In this and in other spectra to follow, the expansions of individual signals are shown so that the signal splitting patterns are recognizable.

    ""
    Figure \(\PageIndex{2}\): The 1H NMR spectrum of 1,1,2-trichloroethane with signal splitting

     

    The signal at 3.96 ppm, corresponding to the two Ha protons, is split into two peaks of equal height (and area) – this is referred to as a doublet. The Hb signal at 5.76 ppm, on the other hand, is split into three peaks, with the middle peak higher than the two outside peaks and the integration ratio between the three peaks is 1:2:1, such splitting signal is called a triplet.

    Signal splitting is caused by spin-spin coupling, a term that describes the magnetic interactions between non-equivalent hydrogen atoms that are with 2 or 3 bonds of the hydrogens producing the signal. The nearby protons have a magnetic moment that can be either against or with the external magnetic field, therefore splitting the energy levels of the protons whose signal is being observed, resulting in the splitting of the signal into multiple peaks (the terms ‘splitting’ and ‘coupling’ are often used interchangeably when discussing NMR).

    The most typical coupling we observed in this course is from non-equivalent vicinal hydrogens that are 3 bonds away, that is, the hydrogens on adjacent carbons. This is also called vicinal coupling or three-bond coupling.

    H NMR couplingFigure \(\PageIndex{3}\): Vicinal Coupling

    A simple rule that applies for predicting the number of peaks (or splitting pattern) expected from coupling, and the rule in 1H NMR is:

    number of peaks = n + 1

    (n is the number of vicinal non-equivalent hydrogens)

     

    We will examine the splitting pattern with different numbers of n:

    • When n=0, the signal is a singlet, or has only one peak, as the signals observed in Figure \(\PageIndex{1}\).
    • When n=1, the signal is a doublet with two peaks. The area ratio of the two peaks for a doublet is 1:1. The space between the two peaks is called coupling constant, Jab, measured in Hz.

    For the example of compound 1,1,2-trichloromethane, the Ha proton signal fits this situation. With only one vicinal proton, Hb, on the adjacent carbon, the signal of Ha shows as a doublet, as observed in Figure \(\PageIndex{4}\).

    Hb spins aligned with bo; deshields Ha, & Hb spin opposed to B0; shields Ha
    Figure \(\PageIndex{4}\): the Ha proton signal of 1,1,2-trichloromethane

     

    • When n=2, the signal is a triplet with three peaks. The three peaks of the triplet have an area ratio of 1:2:1.

    In the same compound, 1,1,2-trichloromethane, the signal of the Hb proton fits into this situation. With two vicinal protons, 2 Ha, on the adjacent carbon, the signal of Hb shows as a triplet, as observed in Figure \(\PageIndex{5}\).

    ""
    Figure \(\PageIndex{5}\): the Hb proton signal of 1,1,2-trichloromethane

     

     
    • When n=3, the signal is a quartet, which means four peaks. The four peaks of the quartet have the area ratio of 1:3:3:1.

    For the spectrum of ethyl acetate (Figure \(\PageIndex{6}\)), the signal of Hb is a quartet, because there are three vicinal protons 3 Hc on the adjacent carbon. Please note that the carbon with Hb connected with oxygen on the other side, and there are no hydrogen atoms on that oxygen atom, so only the coupling with three vicinal protons applies.

    ""
    Figure \(\PageIndex{6}\): The 1H NMR spectrum of ethyl acetate with signals splitting

     

    • When n≥4, the signal can be called a multiplet. Theoretically, with n increasing, the signal is split into more peaks and the total number of peaks is “n+1”. However, the small peaks on the sides may or may not be able to be observed since they might be merged into noise. The signal with more than four peaks is generally called a multiplet, and it is not that critical to tell exactly how many peaks are involved in a multiplet.

    For the spectrum of ethyl acetate (Figure \(\PageIndex{7}\)), the Hc peak in the spectrum of 2-pentanone appears as a sextet, split by the five combined Hb and Hd protons. Technically, this 'sextet' could be considered to be a 'triplet of quartets' with overlapping sub-peaks.

    H-NMR spectrum of 2-pentanone. HA peaks at 1.85 ppm, HB peaks at 2.15 ppm, HC is labeled in red and peaks at 1.35 ppm, and HD peaks ate 0.65 ppm.
    Figure \(\PageIndex{7}\): The 1H NMR spectrum of propyl acetate with signals splitting
     

    Extra notes about signal splitting:

    1. Splitting (coupling) only occurs between nonequivalent protons. For equivalent protons, there is no coupling. In the spectrum of succinic acid (Figure \(\PageIndex{8}\)), for example, the protons on the two middle carbons are equivalent (Ha), so there is no coupling between them, and they show a singlet.
    ""
    Figure \(\PageIndex{8}\): 1H NMR spectrum of succinic acid

    2. Protons in OH or NH generally do not couple with vicinal hydrogens. OH and NH protons are acidic enough to rapidly exchange between different molecules, so the neighboring protons never actually ‘feel’ their influence. See the specific example of 1-heptanol spectrum in Figure \(\PageIndex{9}\):

    ""
    Figure \(\PageIndex{9}\): The 1H NMR spectrum of 1-heptanol
     

     1H NMR Practice

    With the structure of a compound given, we can apply all the knowledge about 1H NMR to assign the signals in the spectrum, that is, to identify which hydrogen(s) a certain signal comes from.

    Worked Example \(\PageIndex{1}\): Signal assignment based on the given structure

    Match the 1H NMR spectrum below to its corresponding compound and assign all signals.

    The spectrum has four signals: triplet (~0.7 ppm), multiplet (~1.4 ppm), singlet ( ~1.9 ppm) and triplet (~2.2 ppm).

    a) cyclopentanone b) 3-pentanone c) butaldehyde

    d) 2-pentanone e) 4-heptanone f) 1-butene

    Approach: It is a good idea to draw the structure of each compound and try to see which matches the spectrum.

    a) 2 signals b) 2 signals c) 4 signals d) 4 signals e) 3 signals f) 4 signals

    The spectrum has four signals: triplet (~0.7 ppm), multiplet (~1.4 ppm), singlet ( ~1.9 ppm) and triplet (~2.2 ppm). Based on the structure of each compound, compounds c), d), and f) should have four signals in the 1H NMR spectrum.

    • There are no signals at about 9 ppm for the aldehyde hydrogen in the spectra, so the spectrum is not for compound c), butaldehyde.
    • There are no signals at about 4~5 ppm for the alkene hydrogens in the spectra, so the spectrum is not for compound f), 1-butene.
    • The signals in the spectrum match what is expected for compound d), 2-pentanone.

    Solution: The spectrum is for 2-pentanone.

    0.7 ppm triplet, 1.4 ppm multiplet, 2.2 ppm triplet, & 1.9 ppm singlet

    Structure Determination based on 1H NMR spectrum

    A lot of valuable information about a compound's structure can be obtained from a 1H NMR spectrum. For a summary, analyzing the four features of the spectrum is critical to elucidate the structure of a compound:

    • The number of signals indicates how many different sets of protons there are in the molecule;
    • The chemical shift of the signal tells us about the electronic environment of each set of protons;
    • The integration under each signal provides information about how many protons there are in the set being measured (keep in mind that the integration values are for the ratio, not the actual number of protons);
    • The splitting pattern of each signal tells about the number of protons on atoms adjacent to the one whose signal is being measured.

    Spin–spin splitting in 1H NMR can be summarized by three rules:

    RULE 1

    Chemically equivalent protons don’t show spin–spin splitting. Equivalent protons may be on the same carbon or on different carbons, but their signals don’t split.

    A structure of chloromethane with text indicating all protons are chemically equivalent, no splitting. A structure of 1,2-dichloroethane with text indicating all protons are chemically equivalent, no splitting.

    RULE 2

    The signal of a proton with n equivalent neighboring protons is split into a multiplet of n + 1 peaks with coupling constant J. Protons that are farther than two carbon atoms apart don’t usually couple. However, they sometimes show weak coupling when they are separated by a \(\pi\) bond.

    First structure labeled splitting observed shows adjacent carbon atoms, each bonded to hydrogen. Second structure labeled splitting not usually observed has 3-carbon chain, hydrogens on non-adjacent carbons.

    RULE 3

    Two groups of protons coupled to each other have the same coupling constant, J.

     

     

    The spectrum of para-methoxypropiophenone in Figure \(\PageIndex{10}\) further illustrates these three rules. The downfield absorptions at 6.91 and 7.93 δ are due to the four aromatic-ring protons. There are two kinds of aromatic protons, each of which gives a signal that is split into a doublet by its neighbor. The –OCH3 signal is unsplit and appears as a sharp singlet at 3.84 δ. The –CH2– protons next to the carbonyl group appear at 2.93 δ in the region expected for protons on carbon next to an unsaturated center, and their signal is split into a quartet by coupling with the protons of the neighboring methyl group. The methyl protons appear as a triplet at 1.20 δ in the usual upfield region.

     

    The H N M R spectrum of para-methoxypropiophenone shows peaks at 0 (T M S), 1.2 (triplet, methyl), 2.9 (quartet, methylene), 3.9 (singlet, methoxy), 6.9 and 7.9 (both doublets, benzene).
    Figure \(\PageIndex{10}\): The 1H NMR spectrum of para-methoxypropiophenone.

     

    Worked Example \(\PageIndex{1}\): Assigning a Chemical Structure from a 1H NMR Spectrum

    Propose a structure for a compound, C5H12O, that fits the following 1H NMR data: 0.92 δ (3 H, triplet, J = 7 Hz), 1.20 δ (6 H, singlet), 1.50 δ (2 H, quartet, J = 7 Hz), 1.64 δ (1 H, broad singlet).

    Strategy

    It’s best to begin solving structural problems by calculating a molecule’s degree of unsaturation. In the present instance, a formula of C5H12O corresponds to a saturated, open-chain molecule, either an alcohol or an ether.

    To interpret the NMR information, let’s look at each absorption individually. The three-proton absorption at 0.92 δ is due to a methyl group in an alkane-like environment, and the triplet-splitting pattern implies that the CH3 is next to a CH2. Thus, our molecule contains an ethyl group, CH3CH2–. The six-proton singlet at 1.20 δ is due to two equivalent alkane-like methyl groups attached to a carbon with no hydrogens, (CH3)2C, and the two-proton quartet at 1.50 δ is due to the CH2 of the ethyl group. All 5 carbons and 11 of the 12 hydrogens in the molecule are now accounted for. The remaining hydrogen, which appears as a broad one-proton singlet at 1.64 δ, is probably due to an OH group, since there is no other way to account for it. Putting the pieces together gives the structure: 2-methyl-2-butanol.

    Solution
    Structure of 2-methyl-2-butanol with shifts for hydrogens on: C 1 and methyl (1.20), O H (1.64), C 3 (1.50), and C 4 (0.92).

     Exercises

    Exercise \(\PageIndex{1}\)

    Predict the splitting patterns you would expect for each proton in the following molecules:

    a. the=    b. The condensed structural formula reads, C H 3 O C H 2 C H 2 B r.   c. The condensed structural formula reads, C l C H 2 C H 2 C H 2 C l.

    d. The condensed structural formula of ethyl isobutyrate.   e. The condensed structural formula of isopropyl propanoate.    f. The structure has a cyclohexene ring fused to a benzene ring; double bond in cyclohexene is opposite fusion.

    Answer
    1. −CHBr2, quartet;  −CH3, doublet
    2. CH3O−, singlet; −OCH2 −, triplet;  −CH2Br, triplet
    3. ClCH2− , triplet; −CH2−, quintet
    4. CH3− , triplet; −CH2− , quartet; −CH− , septet; (CH3)2, doublet
    5. CH3−, triplet; −CH2−, quartet; −CH−, septet; (CH3)2, doublet
    6. =CH, triplet,  −CH2−, doublet, aromatic C−H, two multiplets
    Exercise \(\PageIndex{2}\)

    Draw structures for compounds that meet the following descriptions:

    1. C2H6O; one singlet
    2. C3H7Cl; one doublet and one septet
    3. C4H8Cl2O; two triplets
    4. C4H8O2; one singlet, one triplet, and one quartet
    Answer
    1. CH3OCH3
    2. CH3CH(Cl)CH3
    3. ClCH2CH2OCH2CH2Cl
    4. CH3CH2CO2CH3 or CH3CO2CH2CH3
    Exercise \(\PageIndex{3}\)

    The integrated 1H NMR spectrum of a compound of formula C4H10O is shown below. Propose a structure.

    An integrated 1H NMR spectrum for Problem 11.
    Answer

    CH3CH2OCH2CH3


    This page titled 14.6: ¹H NMR Signal Integration and Splitting is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by Sol Parajon Puenzo (Cañada College) .