Back to chapter

8.20:

¹H NMR: Interpreting Distorted and Overlapping Signals

JoVE 핵심
Analytical Chemistry
JoVE 비디오를 활용하시려면 도서관을 통한 기관 구독이 필요합니다.  전체 비디오를 보시려면 로그인하거나 무료 트라이얼을 시작하세요.
JoVE 핵심 Analytical Chemistry
¹H NMR: Interpreting Distorted and Overlapping Signals

Languages

소셜에 공유하기

The chemical shifts and coupling constant of a spin system can generally be estimated from the spectrum when Δν /J is greater than 10. These are called first-order spin systems, with weakly coupled nuclei. As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The inner line intensities increase at the cost of those of the outer lines, as the signals are slanted or roofed towards each other. When the signals are closer together, and Δν/J is less than 10, the spins are said to be strongly coupled, and the spectra show second-order effects. Peaks may overlap completely and appear like first-order spectra, or result in shoulders and multiplets that cannot be explained simply. Accordingly, computer simulation methods are often used to identify chemical shifts and coupling constants. 

8.20:

¹H NMR: Interpreting Distorted and Overlapping Signals

Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.

As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are slanted or roofed towards each other. When Δν/J is less than 10, the spins are said to be strongly coupled, and the spectra show second-order effects.

Peaks may overlap completely and appear deceptively simple, similar to first-order spectra. Second-order effects can also result in shoulders and multiplets that cannot be interpreted. Accordingly, chemical shifts and coupling constants in these spectra are often identified by computer simulation methods. Because Δν increases with spectrometer frequency and J remains constant, second-order effects decrease when spectra are recorded using higher-field instruments.