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Please be aware that this old REACH registration data factsheet is no longer maintained; it remains frozen as of 19th May 2023.

The new ECHA CHEM database has been released by ECHA, and it now contains all REACH registration data. There are more details on the transition of ECHA's published data to ECHA CHEM here.

Diss Factsheets

Administrative data

Endpoint:
melting point/freezing point
Type of information:
experimental study
Adequacy of study:
key study
Reliability:
2 (reliable with restrictions)

Data source

Reference
Reference Type:
study report
Title:
Unnamed
Year:
2019
Report date:
2019

Materials and methods

Test guideline
Qualifier:
equivalent or similar to guideline
Guideline:
OECD Guideline 102 (Melting point / Melting Range)
Principles of method if other than guideline:
DIN EN ISO 11357-3
GLP compliance:
no
Type of method:
differential scanning calorimetry

Test material

Constituent 1
Chemical structure
Reference substance name:
N-ethylpyridazin-4-amine
EC Number:
846-827-8
Cas Number:
1521274-68-9
Molecular formula:
C6H9N3
IUPAC Name:
N-ethylpyridazin-4-amine
Test material form:
solid: particulate/powder

Results and discussion

Melting / freezing point
Key result
Melting / freezing pt.:
124.6 °C
Atm. press.:
1 013 hPa

Any other information on results incl. tables

Result:

Sample

Tm1

[°C]

Tk*

[°C]

∆m

[%]

4-Pyridazinamine, N-ethyl-

124.6

110.3

1

Explanations

Tm1= melting peak temperature in delivery condition

Tk* = crystallisation temperature

∆m = weight loss, determined at the end of the measurement, based on initial weight

Due to the rounded inlet, an evaluation of the onset temperature does not make sense.
In a first measurement up to 140 ° C showed a strong thermal degradation of the sample with a
Weight loss of about 69%, so for the present measurement a maximum temperature
was chosen just above the melting peak.
* In principle, with a crystalline substance directly below the melting peak, under unfavorable conditions (eg formation of crystallisation germs by soiling, shocks, pressure fluctuations), a spontaneous crystallization can be expected.Under laboratory conditions, a strong hypothermia is often detectable.The sample crystallizes so fast that the heat generated by the crystallization can not be dissipated by the device in the short time, which leads to a "looping" in the course of the curve.In this case, the crystallization peak is to be equated with the beginning of the crystallization.

Applicant's summary and conclusion