Conformational studies by dynamic NMR. V. The stereodynamics of

Nov 1, 1976 - Daniele Casarini, Lodovico Lunazzi, Michele Mancinelli, and Andrea Mazzanti ... Lodovico Lunazzi, Andrea Mazzanti, and Romina Rompietti...
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Conformational Studies by Dynamic NMR. V. 1 The Stereodynamics of Hindered Aliphatic Hydrazones L. Lunazzi,*2aG . Cerioni,2a and K. U. Ingold*2b Contribution f r o m Istituto di Chimica Organica, Unicersitci, Bologna, Italy, and Dicision of Chemistry, National Research Council of Canada, Ottawa, Canada. Receiced February 24, 1976

Abstract: A number of N-ketiminyl-2,2,6,6-tetramethylpiperidines (TMP-N=CR>) have been synthesized and investigated by ‘ H N M R spectroscopy. The piperidyl methyls are either nonequivalent in pairs a t room temperature or become nonequivalent in pairs a t low temperatures. This is shown to be due to restricted rotation about the N-N bond, a phenomenon that is not observed in less hindered hydrazones even at very low temperatures. The free energies of activation for rotation in TMPN=CR2 were determined by line shape analysis. They increase from a low of 7.6 kcal/mol for Rz = H 2 through 1 1.6, 14.35, and 18.0 kcal/mol for R2 = (CH2)4, (CH2)5, and (CH&, respectively. This trend is rationalized in terms of a conformation in which the plane of the N=CR2 moiety is perpendicular to the dynamically averaged plane of the tetramethylpiperidine ring. This conclusion is supported by an x-ray diffraction determination of the structure and conformation of TMP-N=C(CH3)ChHs. The rotational barriers of some N-nitrosoamines are also reported.

The occurrence of restricted rotation around the nitrogennitrogen single bond of N-nitrosoamines, R;N-N=O, is well At room temperature the proton N M R signals due to R’ are usually nonequivalent but they coalesce into averaged signals at higher temperatures. In contrast, a similar nonequivalence of the R’ protons is not observed in the corresponding hydra zone^,^^^^ Rl’N-N=CR2, presumably because there is much less (or no) N - N double bond character in these compounds. We recently discovered” a class of sterically hindered hydrazones which show restricted motion on the N M R time scale a t ambient temperatures. The present paper presents our experimental data on these compounds and discusses their unanticipated stereodynamical behavior.

Results and Discussion All the hydrazones that show evidence of restricted motion in their ‘ H N M R spectra contain the 2,2,6,6-tetramethylpiperidyl (TMP) group. As a typical example, we shall first discuss, in some detail, compound 1 (N-acetoneimineTMP).

Q I

II

N

moiety is coplanar with the “virtual” plane dynamically created in the T M P ring by fast motions 2 and 3 (see below). (ii) The perpendicular conformation in which the moiety A is perpendicular to this plane.

Q I

R,

\/

N

Rl

I

I

R2 (i) coplanar

R? (ii) perpendicular

There are four stereodynamical processes which require consideration: 1. Inversion of the iminyl (sp2)nitrogen in the coplanar conformation can be ruled out since it would make the two ketimino methyls also equivalent a t high temperatures. However, it is found experimentally that these methyls give sharp N M R signals even at 150 “ C (in tolan).

A&-#= I

y R,

forbidden

I

5,n=l 6, n = 2 7, n = 3 8, n = 4 9, n = 5 10, n = 9

R2

L R, R2 = CH3 2,Rl=&=H 3, R, = H;R? = CH, 4, R1 = CH, & = C6H,

/

\ A

Journal of the American Chemical Society

/ 98:24 /

0 1 I

I

N

XC/

At room temperature the IH N M R spectrum (60 MHz) shows two sharp signals due to the ketimino methyls and two broader signals due to the four piperidyl methyls (see Figure 1). On raising the temperature, the ketimino methyl signals remain sharp and nonequivalent, but the piperidyl methyl signals a t first broaden and then coalesce into a single line at 54 O C . The thermodynamic parameters for the process which makes the piperidyl methyls equivalent are given in Table I. There are two possible ground state conformations: (i) The coplanar conformation in which the /N=C

\/

I N

\/

N

2. Inversion of the amino (sp3)nitrogen in the perpendicular conformation is likely to be extremely fast at room temperature. Barriers to nitrogen inversion are known to be quite low1* even in strained rings.I3 It is therefore improbable that inversion of this nitrogen could be responsible for the observed nonequivalence in a six-membered ring a t room temperature.I4 3. Chair-to-chair reversal of the piperidyl ring in the perpendicular conformation is also likely to be very fast a t room temperature. It is known that with piperidine itself this motion can be observed on the N M R time scale only a t -85 Since the four methyl groups on the ring should reduce the barrier for this process we must rule out this motion as the source of our nonequivalence. Further evidence that neither motion 2 nor 3 could produce the observed nonequivalence in the hydrazone comes from

November 24, 1976

0C.14315

7485 Table 1. Thermodynamic Parameters for Motional Averaging in Hydrazones of General Formula TMP-N=CR, (Unless Otherwise Indicated all Data were Obtained at 60 MHz)

AGP~

=CR (1)

7, _/CH,

16.7 t 0.05 16.5 i 0.05

( 2)

7.6 i 0.1 7.5c f 0.1

( 3)

8.9

i

T,, “ C

Eaa

AHfa

ASfb

17.8 f 0.4 17.6 i 0.4

17.2 i 0.4 17.0 i 0.4

1.5 i 1.1 1.4 i 1.2

54.5 53 -122 -121c -91.5C

0.1

36

Solvent

C2C4

A v , Hz

CfY”

23.1 24.0

CHF2C1 CHF,Cl

15.4 26.0C

CHF2C1

30.5C

CDCI,

25.2

CS,

13.5

CDCI,

17.4

(4)

15.6 t 0.1

-OH1

(5)

11.6 i 0.06

12.0 i 0.8

11.5i- 0.8

-0.2

i

3.7