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Caretakers have the weight of the world on their shoulders, but they are often not responsible for their own actions or well-being The ip side of Caretaking is Personal Responsibility Often, the best thing we can do for others is to be fully responsible to and for ourselves We become responsible for our health, our conscious awareness, our results, and our actions The focus moves from others to self



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When RSVP-TE uses CSPF to calculate the path for LSP, the bandwidth consideration is based on the control plane booking information. This bandwidth booking information does not reflect the actual physical link s traffic utilization rate. The reservation, the request, and the CAC are all based on control plane information. For example, if a service uses an LSP with a configured bandwidth of 50 Mbps, the 50 Mbps is signaled and reserved in all routers along the LSP-Path. However, this reservation is on the control plane only. The service can still send 500 Mbps of traffic over the LSP and congest the link. If an LSP is established, it can send any amount of traffic, and the 50 Mbps reservation does not affect the traffic volume. The best way to ensure that the booking reflects reality is to use QoS to enforce the traffic to conform to the booking value. In the same example, the operator can deploy a QoS policy in the service s SAP to police or shape the ingress traffic from the customer to 50 Mbps. Thus, this policy ensures that the service can only send 50 Mbps of traffic to the LSP.





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Personal Responsibility occurs when an individual releases blame and victimization to become fully responsible for his or her life

AGAIN:

What you don t have, you cannot give Personal Responsibility has no room for blame (self or otherwise) By becoming Personally Responsible for our lives we gain the real capacity to care for others We care for others from a position of strength and abundance, not weakness and scarcity We can hold others up without crumbling to the ground from the weight of giving In fact, giving creates a lightness because we understand from experience that we have far more to give than we could have ever imagined Put down the weight of the world and shift the focus to the one place we can control ourselves The focus and attention starts from within before moving out This allows us to see opportunities as they develop DISTINCTION: REACTING VS RESPONDING

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preferentially forwards and backwards with respect to the direction of motion of the ssioning system In this case involving a reaction in which the ssioning system has a signi cant angular momentum ( 36h ), the distribution closely resembles the function 1/sin(u) To understand these distributions, one needs to consider the ssion transition nucleus Figure 1122 shows a coordinate system for describing this nucleus in terms of its quantum numbers J, the total angular momentum M, the projection of J upon a space- xed axis, usually taken to be the direction of motion of the ssioning system, and K, the projection of J upon the nuclear symmetry axis In most collisions, the angular momentum vectors, J, will be concentrated in a plane perpendicular to the beam direction (M 0) In this case, we can easily see a relation between J, K, and the ssion fragment angular distribution.

Reacting is a conscious response to external events There s no room for thinking Someone yells at you, and you yell back That s reacting Responding requires thought Someone yells at you, and you respond by quietly ending the conversation and moving away Responding is a way of taking Personal Responsibility for your thoughts and actions

Consider the case where J K, the nuclear symmetry axis is perpendicular to the beam, and the fragments emerge sidewise to the beam Similarly, if K 0, the symmetry axis of the nucleus is oriented perpendicular to J, that is, along the beam direction, and the fragments are emitted preferentially forward and backward It is this extreme that leads to the 1/sin(u) form [If J is perpendicular to the beam, and the vectors describing the possible directions of the nuclear symmetry axis are uniformly distributed over the surface of a sphere, then the probability of having a symmetry axis at angle u with respect to the beam will go as 1/sin(u).

] For the general case, Wheeler (1963) showed that the probability of emitting a fragment at an angle u from a transition nucleus characterized by J, K, and M is 2pR2 sin u du J J d (u) 2 (11:22) PM,K (u) (2 J 1) M,k 2 4pR The rst term represents a statistical weighting factor, the second term a solid angle factor for the probability of getting the angle u, and the third term is a symmetric top wave function..

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