Abstract

In this paper we derive three equations of motion for a supernova remnant (SNR) in the framework of the thin layer approximation using the Pad\'e approximant. The circumstellar medium is assumed to follow a density profile of either an exponential type, a Gaussian type, or a Lane--Emden ($n=5$) type. The three equations of motion are applied to four SNRs: Tycho, Cas A, Cygnus loop, and SN~1006. The percentage error of the Pad\'e approximated solution is always less than $10\%$. The theoretical decrease of the velocity over ten years for SNRs is evaluated.

Highlights

  • The equation of motion for a supernova remnant (SNR) can be modeled by a single law of motion or multiple laws of motion when the appropriate boundary conditions are provided

  • The three equations of motion are applied to four SNRs: Tycho, Cas A, Cygnus loop, and SN 1006

  • Examples of piece-wise solutions for an SNR can be found in [3]: A first energy conserving phase, r ∝ t0.4 followed by a second adiabatic phase where r ∝ t0.285

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Summary

Introduction

The equation of motion for a supernova remnant (SNR) can be modeled by a single law of motion or multiple laws of motion when the appropriate boundary conditions are provided. Examples of a single law of motion are: The Sedov expansion in the presence of a circumstellar medium (CSM) with constant density where the radius, r, scales as r ∝ t0.4 , see [1], and the momentum conservation in the framework of the thin layer approximation with CSM at constant density where R ∝ t0.25 , see [2]. Examples of piece-wise solutions for an SNR can be found in [3]: A first energy conserving phase, r ∝ t0.4 followed by a second adiabatic phase where r ∝ t0.285. The previous analysis allows posing a basic question: “Is it possible to find an analytical solution for SNRs given the three observable astronomical parameters, age, radius and velocity ?”.

Motion with Exponential Profile
Motion with Gaussian Profile
Motion with the Lane-Emden Profile
Astrophysical Applications
Findings
Conclusion
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